a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models Logo
NPSMEFTd6MFV Class Reference

#include <NPSMEFTd6MFV.h>

+ Inheritance diagram for NPSMEFTd6MFV:

Detailed Description

Definition at line 14 of file NPSMEFTd6MFV.h.

Public Member Functions

virtual bool Init (const std::map< std::string, double > &DPars)
 A method to initialize the model parameters. More...
 
 NPSMEFTd6MFV ()
 
virtual bool PostUpdate ()
 The post-update method for NPSMEFTd6General. More...
 
- Public Member Functions inherited from NPSMEFTd6General
virtual const double A_f (const Particle f) const
 The left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\mathcal{A}_f\). More...
 
virtual const double AFB (const Particle f) const
 The forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(A^f_{FB}\). More...
 
virtual const double alphaMz () const
 The electromagnetic coupling at the \(Z\)-mass scale. More...
 
virtual const double aPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More...
 
virtual const double AuxObs_NP1 () const
 Auxiliary observable AuxObs_NP1 (See code for details.) More...
 
virtual const double AuxObs_NP10 () const
 Auxiliary observable AuxObs_NP10 (See code for details.) More...
 
virtual const double AuxObs_NP11 () const
 Auxiliary observable AuxObs_NP11 (See code for details.) More...
 
virtual const double AuxObs_NP12 () const
 Auxiliary observable AuxObs_NP12 (See code for details.) More...
 
virtual const double AuxObs_NP13 () const
 Auxiliary observable AuxObs_NP13. More...
 
virtual const double AuxObs_NP14 () const
 Auxiliary observable AuxObs_NP14. More...
 
virtual const double AuxObs_NP15 () const
 Auxiliary observable AuxObs_NP15. More...
 
virtual const double AuxObs_NP16 () const
 Auxiliary observable AuxObs_NP16. More...
 
virtual const double AuxObs_NP17 () const
 Auxiliary observable AuxObs_NP17. More...
 
virtual const double AuxObs_NP18 () const
 Auxiliary observable AuxObs_NP18. More...
 
virtual const double AuxObs_NP19 () const
 Auxiliary observable AuxObs_NP19. More...
 
virtual const double AuxObs_NP2 () const
 Auxiliary observable AuxObs_NP2 (See code for details.) More...
 
virtual const double AuxObs_NP20 () const
 Auxiliary observable AuxObs_NP20. More...
 
virtual const double AuxObs_NP21 () const
 Auxiliary observable AuxObs_NP21 (See code for details.) More...
 
virtual const double AuxObs_NP22 () const
 Auxiliary observable AuxObs_NP22 (See code for details.) More...
 
virtual const double AuxObs_NP23 () const
 Auxiliary observable AuxObs_NP23. More...
 
virtual const double AuxObs_NP24 () const
 Auxiliary observable AuxObs_NP24. More...
 
virtual const double AuxObs_NP25 () const
 Auxiliary observable AuxObs_NP25. More...
 
virtual const double AuxObs_NP26 () const
 Auxiliary observable AuxObs_NP26. More...
 
virtual const double AuxObs_NP27 () const
 Auxiliary observable AuxObs_NP27. More...
 
virtual const double AuxObs_NP28 () const
 Auxiliary observable AuxObs_NP28. More...
 
virtual const double AuxObs_NP29 () const
 Auxiliary observable AuxObs_NP29. More...
 
virtual const double AuxObs_NP3 () const
 Auxiliary observable AuxObs_NP3 (See code for details.) More...
 
virtual const double AuxObs_NP30 () const
 Auxiliary observable AuxObs_NP30. More...
 
virtual const double AuxObs_NP4 () const
 Auxiliary observable AuxObs_NP4 (See code for details.) More...
 
virtual const double AuxObs_NP5 () const
 Auxiliary observable AuxObs_NP5 (See code for details.) More...
 
virtual const double AuxObs_NP6 () const
 Auxiliary observable AuxObs_NP6 (See code for details.) More...
 
virtual const double AuxObs_NP7 () const
 Auxiliary observable AuxObs_NP7 (See code for details.) More...
 
virtual const double AuxObs_NP8 () const
 Auxiliary observable AuxObs_NP8 (See code for details.) More...
 
virtual const double AuxObs_NP9 () const
 Auxiliary observable AuxObs_NP9 (See code for details.) More...
 
virtual const double bPskPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More...
 
virtual const double Br_H_exo () const
 The branching ratio of the of the Higgs into exotic particles. More...
 
virtual const double Br_H_inv () const
 The branching ratio of the of the Higgs into invisible particles. More...
 
virtual const double Br_H_inv_NP () const
 The branching ratio of the of the Higgs into invisible particles (only invisible new particles). More...
 
virtual const double BrH2d2dRatio () const
 The ratio of the Br \((H\to 2d2d)\) in the current model and in the Standard Model. More...
 
virtual const double BrH2e2muRatio () const
 The ratio of the Br \((H\to 2e 2\mu)\) in the current model and in the Standard Model. More...
 
virtual const double BrH2e2vRatio () const
 The ratio of the Br \((H\to 2e2v)\) in the current model and in the Standard Model. More...
 
virtual const double BrH2evRatio () const
 The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model. More...
 
virtual const double BrH2L2dRatio () const
 The ratio of the Br \((H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
virtual const double BrH2L2LRatio () const
 The ratio of the Br \((H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
virtual const double BrH2L2uRatio () const
 The ratio of the Br \((H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
virtual const double BrH2L2v2Ratio () const
 The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More...
 
virtual const double BrH2L2vRatio () const
 The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
virtual const double BrH2l2vRatio () const
 The ratio of the Br \((H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More...
 
virtual const double BrH2Lv2Ratio () const
 The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More...
 
virtual const double BrH2LvRatio () const
 The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
virtual const double BrH2mu2vRatio () const
 The ratio of the Br \((H\to 2\mu 2v)\) in the current model and in the Standard Model. More...
 
virtual const double BrH2muvRatio () const
 The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model. More...
 
virtual const double BrH2u2dRatio () const
 The ratio of the Br \((H\to 2u2d)\) in the current model and in the Standard Model. More...
 
virtual const double BrH2u2uRatio () const
 The ratio of the Br \((H\to 2u2u)\) in the current model and in the Standard Model. More...
 
virtual const double BrH2udRatio () const
 The ratio of the Br \((H\to 2ud)\) in the current model and in the Standard Model. More...
 
virtual const double BrH2v2dRatio () const
 The ratio of the Br \((H\to 2v2d)\) in the current model and in the Standard Model. More...
 
virtual const double BrH2v2uRatio () const
 The ratio of the Br \((H\to 2v2u)\) in the current model and in the Standard Model. More...
 
virtual const double BrH2v2vRatio () const
 The ratio of the Br \((H\to 2v2v)\) in the current model and in the Standard Model. More...
 
virtual const double BrH4dRatio () const
 The ratio of the Br \((H\to 4d)\) in the current model and in the Standard Model. More...
 
virtual const double BrH4eRatio () const
 The ratio of the Br \((H\to 4e)\) in the current model and in the Standard Model. More...
 
virtual const double BrH4fCCRatio () const
 The ratio of the Br \((H\to 4f, CC)\) in the current model and in the Standard Model. More...
 
virtual const double BrH4fNCRatio () const
 The ratio of the Br \((H\to 4f, NC)\) in the current model and in the Standard Model. More...
 
virtual const double BrH4fRatio () const
 The ratio of the Br \((H\to 4f)\) in the current model and in the Standard Model. More...
 
virtual const double BrH4L2Ratio () const
 The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More...
 
virtual const double BrH4LRatio () const
 The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
virtual const double BrH4lRatio () const
 The ratio of the Br \((H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More...
 
virtual const double BrH4muRatio () const
 The ratio of the Br \((H\to 4\mu)\) in the current model and in the Standard Model. More...
 
virtual const double BrH4uRatio () const
 The ratio of the Br \((H\to 4u)\) in the current model and in the Standard Model. More...
 
virtual const double BrH4vRatio () const
 The ratio of the Br \((H\to 4v)\) in the current model and in the Standard Model. More...
 
virtual const double BrHbbRatio () const
 The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model. More...
 
virtual const double BrHccRatio () const
 The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model. More...
 
virtual const double BrHevmuvRatio () const
 The ratio of the Br \((H\to e\nu \mu\nu)\) in the current model and in the Standard Model. More...
 
virtual const double BrHgagaRatio () const
 The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model. More...
 
virtual const double BrHggRatio () const
 The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model. More...
 
virtual const double BrHll_vvorjjRatio () const
 The ratio of the Br \((H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More...
 
virtual const double BrHlv_lvorjjRatio () const
 The ratio of the Br \((H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More...
 
virtual const double BrHlvjjRatio () const
 The ratio of the Br \((H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More...
 
virtual const double BrHLvudRatio () const
 The ratio of the Br \((H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
virtual const double BrHLvvLRatio () const
 The ratio of the Br \((H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
virtual const double BrHmumuRatio () const
 The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model. More...
 
virtual const double BrHssRatio () const
 The ratio of the Br \((H\to s\bar{s})\) in the current model and in the Standard Model. More...
 
virtual const double BrHtautauRatio () const
 The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More...
 
virtual const double BrHtoinvRatio () const
 The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model. More...
 
virtual const double BrHudduRatio () const
 The ratio of the Br \((H\to uddu)\) in the current model and in the Standard Model. More...
 
virtual const double BrHvisRatio () const
 The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model. More...
 
virtual const double BrHVVRatio () const
 The ratio of the Br \((H\to VV)\) in the current model and in the Standard Model. More...
 
virtual const double BrHWffRatio () const
 The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual const double BrHWjjRatio () const
 The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model. More...
 
virtual const double BrHWlvRatio () const
 The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual const double BrHWW2l2vRatio () const
 The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual const double BrHWW4fRatio () const
 The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual const double BrHWW4jRatio () const
 The ratio of the Br \((H\to WW^*\to 4j)\) in the current model and in the Standard Model. More...
 
virtual const double BrHWWRatio () const
 The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model. More...
 
virtual const double BrHZddRatio () const
 The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
virtual const double BrHZffRatio () const
 The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual const double BrHZgaeeRatio () const
 The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model. More...
 
virtual const double BrHZgallRatio () const
 The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual const double BrHZgamumuRatio () const
 The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model. More...
 
virtual const double BrHZgaRatio () const
 The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model. More...
 
virtual const double BrHZllRatio () const
 The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual const double BrHZuuRatio () const
 The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
virtual const double BrHZvvRatio () const
 The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model. More...
 
virtual const double BrHZZ2e2muRatio () const
 The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model. More...
 
virtual const double BrHZZ4dRatio () const
 The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
virtual const double BrHZZ4eRatio () const
 The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More...
 
virtual const double BrHZZ4fRatio () const
 The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
virtual const double BrHZZ4lRatio () const
 The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
virtual const double BrHZZ4muRatio () const
 The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More...
 
virtual const double BrHZZ4uRatio () const
 The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
virtual const double BrHZZ4vRatio () const
 The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More...
 
virtual const double BrHZZRatio () const
 The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model. More...
 
virtual const double BrW (const Particle fi, const Particle fj) const
 The branching ratio of the \(W\) boson decaying into a SM fermion pair, \(Br(W\to f_i f_j)\). More...
 
virtual const double cbW_TWG (const double mu) const
 
const double CeeLL_bottom (const double mu) const
 
const double CeeLL_charm (const double mu) const
 
const double CeeLL_down (const double mu) const
 
const double CeeLL_e (const double mu) const
 
const double CeeLL_mu (const double mu) const
 
const double CeeLL_strange (const double mu) const
 
const double CeeLL_tau (const double mu) const
 
const double CeeLL_top (const double mu) const
 
const double CeeLL_up (const double mu) const
 
const double CeeLR_bottom (const double mu) const
 
const double CeeLR_charm (const double mu) const
 
const double CeeLR_down (const double mu) const
 
const double CeeLR_e (const double mu) const
 
const double CeeLR_mu (const double mu) const
 
const double CeeLR_strange (const double mu) const
 
const double CeeLR_tau (const double mu) const
 
const double CeeLR_top (const double mu) const
 
const double CeeLR_up (const double mu) const
 
const double CeeRL_bottom (const double mu) const
 
const double CeeRL_charm (const double mu) const
 
const double CeeRL_down (const double mu) const
 
const double CeeRL_e (const double mu) const
 
const double CeeRL_mu (const double mu) const
 
const double CeeRL_strange (const double mu) const
 
const double CeeRL_tau (const double mu) const
 
const double CeeRL_top (const double mu) const
 
const double CeeRL_up (const double mu) const
 
const double CeeRR_bottom (const double mu) const
 
const double CeeRR_charm (const double mu) const
 
const double CeeRR_down (const double mu) const
 
const double CeeRR_e (const double mu) const
 
const double CeeRR_mu (const double mu) const
 
const double CeeRR_strange (const double mu) const
 
const double CeeRR_tau (const double mu) const
 
const double CeeRR_top (const double mu) const
 
const double CeeRR_up (const double mu) const
 
virtual const double CEWHd11 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{11}\). More...
 
virtual const double CEWHd22 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{22}\). More...
 
virtual const double CEWHd33 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{33}\). More...
 
virtual const double CEWHdbb () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{bb}\). More...
 
virtual const double CEWHddd () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{dd}\). More...
 
virtual const double CEWHdss () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{ss}\). More...
 
virtual const double CEWHe11 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{11}\). More...
 
virtual const double CEWHe22 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{22}\). More...
 
virtual const double CEWHe33 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{33}\). More...
 
virtual const double CEWHL111 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{11}\). More...
 
virtual const double CEWHL122 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{22}\). More...
 
virtual const double CEWHL133 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{33}\). More...
 
virtual const double CEWHL311 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{11}\). More...
 
virtual const double CEWHL322 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{22}\). More...
 
virtual const double CEWHL333 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{33}\). More...
 
virtual const double CEWHQ111 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{11}\). More...
 
virtual const double CEWHQ122 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{22}\). More...
 
virtual const double CEWHQ133 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{33}\). More...
 
virtual const double CEWHQ1bb () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{bb}\). More...
 
virtual const double CEWHQ1cc () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{cc}\). More...
 
virtual const double CEWHQ1dd () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{dd}\). More...
 
virtual const double CEWHQ1ss () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{ss}\). More...
 
virtual const double CEWHQ1tt () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{tt}\). More...
 
virtual const double CEWHQ1uu () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{uu}\). More...
 
virtual const double CEWHQ311 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{11}\). More...
 
virtual const double CEWHQ322 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{22}\). More...
 
virtual const double CEWHQ333 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{33}\). More...
 
virtual const double CEWHQ3bb () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{bb}\). More...
 
virtual const double CEWHQ3cc () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{cc}\). More...
 
virtual const double CEWHQ3dd () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{dd}\). More...
 
virtual const double CEWHQ3ss () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{ss}\). More...
 
virtual const double CEWHQ3tt () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{tt}\). More...
 
virtual const double CEWHQ3uu () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{uu}\). More...
 
virtual const double CEWHQd33 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(d)})_{33}\). More...
 
virtual const double CEWHQu33 () const
 Combination of coefficients of the Warsaw basis not constrained by EWPO (at LO) \((\hat{C}_{HQ}^{(u)})_{33}\). More...
 
virtual const double CEWHu11 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{11}\). More...
 
virtual const double CEWHu22 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{22}\). More...
 
virtual const double CEWHu33 () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{33}\). More...
 
virtual const double CEWHucc () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{cc}\). More...
 
virtual const double CEWHutt () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{tt}\). More...
 
virtual const double CEWHuuu () const
 Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{uu}\). More...
 
virtual const double cgaga_HB (const double mu) const
 The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double cgg_HB (const double mu) const
 The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double cggEff_HB (const double mu) const
 The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double cHb_TWG (const double mu) const
 
const double chi2FCChh4Top () const
 
const double chi2FCChhbbcc () const
 
const double chi2FCChhee () const
 
const double chi2FCChhenu () const
 
const double chi2FCChhHtt () const
 
const double chi2FCChhHW () const
 
const double chi2FCChhjj () const
 
const double chi2FCChhmumu () const
 
const double chi2FCChhmunu () const
 
const double chi2FCChhtanu () const
 
const double chi2FCChhtata () const
 
const double chi2FCChhtb () const
 
const double chi2FCChhtt () const
 
const double chi2FCChhWW () const
 
const double chi2FCChhZtt () const
 
virtual const double cHQ3_TWG (const double mu) const
 
virtual const double cHQm_TWG (const double mu) const
 
virtual const double cHQp_TWG (const double mu) const
 
virtual const double cHt_TWG (const double mu) const
 
virtual const double cHtb_TWG (const double mu) const
 
virtual const double computeGammaTotalRatio () const
 The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More...
 
virtual const double cQd1_TWG (const double mu) const
 
virtual const double cQd8_TWG (const double mu) const
 
virtual const double cQe_TWG (const double mu) const
 
virtual const double cQl3_TWG (const double mu) const
 
virtual const double cQlM_TWG (const double mu) const
 
virtual const double cQlP_TWG (const double mu) const
 
virtual const double cQq11_TWG (const double mu) const
 
virtual const double cQq18_TWG (const double mu) const
 
virtual const double cQQ1_TWG (const double mu) const
 
virtual const double cQq31_TWG (const double mu) const
 
virtual const double cQq38_TWG (const double mu) const
 
virtual const double cQQ8_TWG (const double mu) const
 
virtual const double cQt1_TWG (const double mu) const
 
virtual const double cQt8_TWG (const double mu) const
 
virtual const double cQu1_TWG (const double mu) const
 
virtual const double cQu8_TWG (const double mu) const
 
virtual const double ctd1_TWG (const double mu) const
 
virtual const double ctd8_TWG (const double mu) const
 
virtual const double cte_TWG (const double mu) const
 
virtual const double ctG_TWG (const double mu) const
 
virtual const double ctH_TWG (const double mu) const
 
virtual const double ctl_TWG (const double mu) const
 
virtual const double ctlS_TWG (const double mu) const
 
virtual const double ctlT_TWG (const double mu) const
 
virtual const double ctq1_TWG (const double mu) const
 
virtual const double ctq8_TWG (const double mu) const
 
virtual const double ctt1_TWG (const double mu) const
 
virtual const double ctu1_TWG (const double mu) const
 
virtual const double ctu8_TWG (const double mu) const
 
virtual const double ctW_TWG (const double mu) const
 
virtual const double ctZ_TWG (const double mu) const
 
virtual const double cZBox_HB (const double mu) const
 The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double cZga_HB (const double mu) const
 The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double cZZ_HB (const double mu) const
 The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double del_A_mu (const double mu) const
 Correction to photon WF. More...
 
virtual const double del_e_mu (const double mu) const
 Correction to electric charge. More...
 
virtual const double del_sW2_mu (const double mu) const
 Correction to (sin squared of) weak mixing angle. More...
 
virtual const double del_Z_mu (const double mu) const
 Correction to Z WF. More...
 
virtual const double del_ZA_mu (const double mu) const
 Correction to Z-A mixing. More...
 
virtual const double delQ_gNC (const double mu) const
 Separate, charge-proportional, indirect correction to EW neutral currents. More...
 
virtual const double delta2sBRH3 (const double C1prod, const double C1Hxx) const
 Quadratic contribution from the Higgs self-couplings modifications to the signal strength for \(\sigma \times BR(H\to xx)\) in the current model. More...
 
virtual const double delta2sH3 (const double C1) const
 Quadratic contribution from the Higgs self-couplings modifications to the signal strength for an observable \(\sigma\) in the current model. More...
 
virtual const double delta_AFB_ee (const double pol_e, const double pol_p, const double s) const
 
virtual const double delta_AFB_f (const Particle f, const double pol_e, const double pol_p, const double s) const
 
virtual const double delta_alrmoller (const double q2, const double y) const
 The computation of the parity violating asymmetry in Moller scattering. More...
 
virtual const double delta_amuon () const
 The computation of the anomalous magnetic moment of the muon \(a_\mu=(g_\mu-2)/2\). More...
 
virtual const double delta_Dsigma_f (const Particle f, const double pol_e, const double pol_p, const double s, const double cos) const
 
virtual const double delta_gAnue () const
 The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gAnue. More...
 
virtual const double delta_gLnuN2 () const
 The computation of the correction to the effective neutrino nucleon LH coupling: delta_gLnuN2. More...
 
virtual const double delta_gRnuN2 () const
 The computation of the correction to the effective neutrino nucleon RH coupling: delta_gRnuN2. More...
 
virtual const double delta_gVnue () const
 The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gVnue. More...
 
virtual const double delta_mubbH_1 (const double sqrt_s) const
 The SMEFT linear correction to the ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_mubbH_2 (const double sqrt_s) const
 The SMEFT quadratic correction to the ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_muggH_1 (const double sqrt_s) const
 The SMEFT linear correction to the ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_muggH_2 (const double sqrt_s) const
 The SMEFT quadratic correction to the ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_mutH_1 (const double sqrt_s) const
 The SMEFT linear correction to the ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_mutH_2 (const double sqrt_s) const
 The SMEFT quadratic correction to the ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_muttH_1 (const double sqrt_s) const
 The SMEFT linear correction to the ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_muttH_2 (const double sqrt_s) const
 The SMEFT quadratic correction to the ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_muVBF_1 (const double sqrt_s) const
 The SMEFT linear correction to the ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_muVBF_2 (const double sqrt_s) const
 The SMEFT quadratic correction to the ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_muVH_1 (const double sqrt_s) const
 The SMEFT linear correction to the ratio \(\mu_{VH}\) between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_muVH_2 (const double sqrt_s) const
 The SMEFT quadratic correction to the ratio \(\mu_{VH}\) between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_muWH_1 (const double sqrt_s) const
 The SMEFT linear correction to the ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_muWH_2 (const double sqrt_s) const
 The SMEFT quadratic correction to the ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_muZH_1 (const double sqrt_s) const
 The SMEFT linear correction to the ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_muZH_2 (const double sqrt_s) const
 The SMEFT quadratic correction to the ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double delta_Qwemoller (const double q2, const double y) const
 The computation of the electron's weak charge. More...
 
virtual const double delta_Qwn () const
 The computation of the neutron weak charge: Qwn. More...
 
virtual const double delta_Qwp () const
 The computation of the proton weak charge: Qwp. More...
 
virtual const double delta_sigma_ee (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const
 
virtual const double delta_sigma_f (const Particle f, const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const
 
virtual const double delta_sigma_had (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const
 
virtual const double delta_sigmaTot_ee (const double pol_e, const double pol_p, const double s) const
 
virtual const double delta_sigmaTot_f (const Particle f, const double pol_e, const double pol_p, const double s) const
 
virtual const double delta_TauLFU_gmuge () const
 The computation of the correction to the LFU ratio \(g_\mu/ g_e \). More...
 
virtual const double delta_TauLFU_gtauge () const
 The computation of the correction to the LFU ratio \(g_\tau/ g_e \). More...
 
virtual const double delta_TauLFU_gtaugmu () const
 The computation of the correction to the LFU ratio \(g_\tau/ g_\mu \). More...
 
virtual const double delta_TauLFU_gtaugmuK () const
 The computation of the correction to the LFU ratio \(\left(g_\tau/ g_\mu\right)_K \). More...
 
virtual const double delta_TauLFU_gtaugmuPi () const
 The computation of the correction to the LFU ratio \(\left(g_\tau/ g_\mu\right)_\pi \). More...
 
virtual const double deltaa0 () const
 The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltaa02 () const
 The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltaA_f (const Particle f) const
 The new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta \mathcal{A}_f\). More...
 
virtual const double deltaAFB (const Particle f) const
 The new physics contribution to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta A^f_{FB}\). More...
 
virtual const double deltaaMZ () const
 The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltaaMZ2 () const
 The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltaaSMZ () const
 The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltaaSMZ2 () const
 The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltacZ_HB (const double mu) const
 The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double deltadxsdcoseeWWlvjjLEP2 (const double sqrt_s, const int bin) const
 The new physics contribution to the differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph]. More...
 
virtual const double deltaeNP (const double mu) const
 The new physics relative contribution to the EW coupling constant \(e\). More...
 
virtual const double deltaG1_hWW () const
 The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More...
 
virtual const double deltaG1_hWW_mu (const double mu) const
 The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More...
 
virtual const double deltaG1_hZA () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More...
 
virtual const double deltaG1_hZA_mu (const double mu) const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More...
 
virtual const double deltaG1_hZARatio () const
 The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
virtual const double deltaG1_hZARatio_mu (const double mu) const
 The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
virtual const double deltaG1_hZZ () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More...
 
virtual const double deltaG1_hZZ_mu (const double mu) const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More...
 
virtual const double deltag1gaNP (const double mu) const
 The new physics contribution to the anomalous triple gauge coupling \(g_{1,\gamma}\). More...
 
virtual const double deltag1ZNP (const double mu) const
 The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More...
 
virtual const double deltag1ZNPEff () const
 The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More...
 
virtual const double deltaG2_hWW () const
 The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More...
 
virtual const double deltaG2_hWW_mu (const double mu) const
 The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More...
 
virtual const double deltaG2_hZA () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More...
 
virtual const double deltaG2_hZA_mu (const double mu) const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More...
 
virtual const double deltaG2_hZZ () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More...
 
virtual const double deltaG2_hZZ_mu (const double mu) const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More...
 
virtual const double deltaG3_hWW () const
 The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More...
 
virtual const double deltaG3_hWW_mu (const double mu) const
 The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More...
 
virtual const double deltaG3_hZZ () const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More...
 
virtual const double deltaG3_hZZ_mu (const double mu) const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More...
 
const double deltag3G () const
 The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\). More...
 
gslpp::complex deltaG_Aff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). More...
 
gslpp::complex deltaG_Gff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu}^A \bar{f}\sigma^{\mu\nu} T_A f\). More...
 
virtual const double deltaG_hAA () const
 The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More...
 
virtual const double deltaG_hAA_mu (const double mu) const
 The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More...
 
virtual const double deltaG_hAARatio () const
 The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
virtual const double deltaG_hAARatio_mu (const double mu) const
 The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
gslpp::complex deltaG_hAff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). More...
 
virtual gslpp::complex deltaG_hff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More...
 
virtual gslpp::complex deltaG_hff_mu (const Particle p, const double mu) const
 The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More...
 
gslpp::complex deltaG_hGff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). More...
 
virtual const double deltaG_hgg () const
 The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More...
 
virtual const double deltaG_hgg_mu (const double mu) const
 The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More...
 
virtual const double deltaG_hggRatio () const
 The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
virtual const double deltaG_hggRatio_mu (const double mu) const
 The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More...
 
virtual const double deltaG_hhhRatio () const
 The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More...
 
virtual const double deltaG_hhhRatio_mu (const double mu) const
 The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More...
 
gslpp::complex deltaG_hZff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). More...
 
gslpp::complex deltaG_Zff (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigma^{\mu\nu} f\). More...
 
virtual const double deltaGA_f (const Particle p) const
 New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More...
 
virtual const double deltaGamma_W () const
 The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\). More...
 
virtual const double deltaGamma_Wff (const Particle fi, const Particle fj) const
 The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More...
 
virtual const double deltaGamma_Z () const
 The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\). More...
 
virtual const double deltaGamma_Zf (const Particle f) const
 The new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More...
 
const double deltaGammaH2d2dRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2d2dRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2e2muRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2e2muRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2e2vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2e2vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2evRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2evRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2L2dRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2L2dRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2L2LRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2L2LRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2L2uRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2L2uRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2L2v2Ratio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2L2v2Ratio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2L2vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2l2vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2L2vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2l2vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2Lv2Ratio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2Lv2Ratio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2LvRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2LvRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2mu2vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2mu2vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2muvRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2muvRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2u2dRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2u2dRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2u2uRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2u2uRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2udRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2udRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2v2dRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2v2dRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2v2uRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2v2uRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2v2vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH2v2vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4dRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4dRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4eRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4eRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4fCCRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4f, CC)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4fCCRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4f, CC)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4fNCRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4f, NC)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4fNCRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4f, NC)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4fRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4fRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4L2Ratio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4L2Ratio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4LRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4lRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4LRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4lRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4muRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4muRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4uRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4uRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaH4vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHbbRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHbbRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHccRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHccRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHevmuvRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHevmuvRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHffRatio1 (const double mf, const double CifH) const
 The ratio of the \(\Gamma(H\to ff)\) in the current model and in the Standard Model. More...
 
const double deltaGammaHffRatio2 (const double mf, const double CifH) const
 The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the ratio of the \(\Gamma(H\to ff)\) in the current model and in the Standard Model at order Lambd. More...
 
const double deltaGammaHgagaRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHgagaRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHggRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...
 
const double deltaGammaHggRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHll_vvorjjRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHll_vvorjjRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHlv_lvorjjRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHlv_lvorjjRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHlvjjRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHlvjjRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHLvudRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHLvudRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHLvvLRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHLvvLRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHmumuRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHmumuRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHssRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ss)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHssRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ss)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHtautauRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHtautauRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHudduRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHudduRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWffRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWffRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWjjRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWjjRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWlvRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWlvRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWW2l2vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWW2l2vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWW4fRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWW4fRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWW4jRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWW4jRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWWRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHWWRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZddRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZddRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZeeRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZeeRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZffRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZffRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZgaRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZgaRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZllRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZllRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZmumuRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZmumuRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZuuRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZuuRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZvvRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZvvRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ2e2muRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ2e2muRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4dRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4dRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4eRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4eRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4fRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4fRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4lRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4lRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4muRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4muRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4uRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4uRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4vRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZ4vRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More...
 
const double deltaGammaHZZRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More...
 
virtual const double deltaGammaTotalRatio1 () const
 The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More...
 
virtual const double deltaGammaTotalRatio1noError () const
 The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors. More...
 
virtual const double deltaGammaTotalRatio2 () const
 The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients. More...
 
virtual const double DeltaGF () const
 New physics contribution to the Fermi constant. More...
 
const double deltaGL_f (const Particle p) const
 New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More...
 
const double deltaGL_f_mu (const Particle p, const double mu) const
 New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More...
 
virtual gslpp::complex deltaGL_Wff (const Particle pbar, const Particle p) const
 New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More...
 
virtual gslpp::complex deltaGL_Wff_mu (const Particle pbar, const Particle p, const double mu) const
 New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More...
 
gslpp::complex deltaGL_Wffh (const Particle pbar, const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\). More...
 
const double deltaGL_Zffh (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\). More...
 
virtual const double deltaGmu () const
 The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltaGmu2 () const
 The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
const double deltaGR_f (const Particle p) const
 New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More...
 
const double deltaGR_f_mu (const Particle p, const double mu) const
 New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More...
 
virtual gslpp::complex deltaGR_Wff (const Particle pbar, const Particle p) const
 New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More...
 
virtual gslpp::complex deltaGR_Wff_mu (const Particle pbar, const Particle p, const double mu) const
 New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More...
 
gslpp::complex deltaGR_Wffh (const Particle pbar, const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\). More...
 
const double deltaGR_Zffh (const Particle p) const
 The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\). More...
 
virtual const double deltaGV_f (const Particle p) const
 New physics contribution to the neutral-current vector coupling \(g_V^f\). More...
 
virtual const double deltaGwd6 () const
 The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\). More...
 
virtual const double deltaGwd62 () const
 The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\). More...
 
virtual const double deltaGzd6 () const
 The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\). More...
 
virtual const double deltaGzd62 () const
 The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\). More...
 
virtual const double deltaH3L1 (double C1) const
 The coefficient of the 1-loop linear term in the Higgs selfcoupling. More...
 
virtual const double deltaH3L2 (double C1) const
 The coefficient of the 1-loop quadratic term in the Higgs selfcoupling. More...
 
virtual const double deltaKgammaNP (const double mu) const
 The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\). More...
 
virtual const double deltaKgammaNPEff () const
 The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More...
 
virtual const double deltaKZNP (const double mu) const
 The new physics contribution to the anomalous triple gauge coupling \(\kappa_{Z}\). More...
 
virtual const double deltamb () const
 The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltamb2 () const
 The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltamc () const
 The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltamc2 () const
 The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltaMh () const
 The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltaMh2 () const
 The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
const double deltaMLL2_f (const Particle f, const double s, const double t) const
 
const double deltaMLR2_f (const Particle f, const double s) const
 
const double deltaMLR2t_e (const double s, const double t) const
 
const double deltaMRL2_f (const Particle f, const double s) const
 
const double deltaMRL2t_e (const double s, const double t) const
 
const double deltaMRR2_f (const Particle f, const double s, const double t) const
 
virtual const double deltamt () const
 The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltamt2 () const
 The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltamtau () const
 The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltamtau2 () const
 The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltaMw () const
 The relative correction to the mass of the \(W\) boson, \(\delta M_W/M_W\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltaMw2 () const
 The relative correction to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltaMwd6 () const
 The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\). More...
 
virtual const double deltaMwd62 () const
 The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\). More...
 
virtual const double deltaMz () const
 The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double deltaMz2 () const
 The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More...
 
virtual const double DeltaOalphtoW (const double dOSMdalpha, const double mu) const
 Difference in prediction in \(\alpha\) scheme and W mass scheme, computed from observable in \(\alpha\) scheme. Difference at tree level. More...
 
virtual const double DeltaOWtoalph (const double dOSMdMW, const double mu) const
 Difference in prediction in \(\alpha\) scheme and W mass scheme, computed from observable in W mass scheme. Difference at tree level. More...
 
virtual const double deltaR0_f (const Particle f) const
 The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More...
 
virtual const double deltaSigmaHadron () const
 The new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\delta \sigma_h^0\). More...
 
virtual const double deltaxseeWW4fLEP2 (const double sqrt_s, const int fstate) const
 The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More...
 
virtual const double deltaxseeWWtotLEP2 (const double sqrt_s) const
 The new physics contribution to the total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More...
 
virtual const double deltayb_HB (const double mu) const
 The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double deltayc_HB (const double mu) const
 The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double deltaymu_HB (const double mu) const
 The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double deltays_HB (const double mu) const
 The Higgs-basis coupling \(\delta y_s\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double deltayt_HB (const double mu) const
 The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double deltaytau_HB (const double mu) const
 The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double delU_gCC (const double mu) const
 Universal indirect correction to EW charged currents. More...
 
virtual const double delU_gNC (const double mu) const
 Universal indirect correction to EW neutral currents. More...
 
virtual const double dxsdcoseeWWlvjjLEP2 (const double sqrt_s, const int bin) const
 The differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph]. More...
 
virtual const double dxseeWWdcos (const double sqrt_s, const double cos) const
 The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle. More...
 
virtual const double dxseeWWdcosBin (const double sqrt_s, const double cos1, const double cos2) const
 The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle. More...
 
virtual const double Gamma_Z () const
 The total decay width of the \(Z\) boson, \(\Gamma_Z\). More...
 
virtual const double Gamma_Zf (const Particle f) const
 The decay width of the \(Z\) boson into a given fermion pair, \(\Gamma_Z^{f}\). More...
 
const double GammaH2d2dRatio () const
 The ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. More...
 
const double GammaH2e2muRatio () const
 The ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. More...
 
const double GammaH2e2vRatio () const
 The ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. More...
 
const double GammaH2evRatio () const
 The ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. More...
 
const double GammaH2L2dRatio () const
 The ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
const double GammaH2L2LRatio () const
 The ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
const double GammaH2L2uRatio () const
 The ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
const double GammaH2L2v2Ratio () const
 The ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More...
 
const double GammaH2L2vRatio () const
 The ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
const double GammaH2l2vRatio () const
 The ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More...
 
const double GammaH2Lv2Ratio () const
 The ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More...
 
const double GammaH2LvRatio () const
 The ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
const double GammaH2mu2vRatio () const
 The ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. More...
 
const double GammaH2muvRatio () const
 The ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. More...
 
const double GammaH2u2dRatio () const
 The ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. More...
 
const double GammaH2u2uRatio () const
 The ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. More...
 
const double GammaH2udRatio () const
 The ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. More...
 
const double GammaH2v2dRatio () const
 The ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. More...
 
const double GammaH2v2uRatio () const
 The ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. More...
 
const double GammaH2v2vRatio () const
 The ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. More...
 
const double GammaH4dRatio () const
 The ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. More...
 
const double GammaH4eRatio () const
 The ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. More...
 
const double GammaH4fCCRatio () const
 The ratio of the \(\Gamma(H\to 4f)\) via CC in the current model and in the Standard Model. More...
 
const double GammaH4fNCRatio () const
 The ratio of the \(\Gamma(H\to 4f)\) via NC in the current model and in the Standard Model. More...
 
const double GammaH4fRatio () const
 The ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. More...
 
const double GammaH4L2Ratio () const
 The ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More...
 
const double GammaH4LRatio () const
 The ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
const double GammaH4lRatio () const
 The ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More...
 
const double GammaH4muRatio () const
 The ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. More...
 
const double GammaH4uRatio () const
 The ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. More...
 
const double GammaH4vRatio () const
 The ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. More...
 
const double GammaHbbRatio () const
 The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. More...
 
const double GammaHccRatio () const
 The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. More...
 
const double GammaHevmuvRatio () const
 The ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. More...
 
const double GammaHgagaRatio () const
 The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. More...
 
const double GammaHggRatio () const
 The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. More...
 
const double GammaHll_vvorjjRatio () const
 The ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More...
 
const double GammaHlv_lvorjjRatio () const
 The ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More...
 
const double GammaHlvjjRatio () const
 The ratio of the \(\Gamma(H\to l l j j)\) ( \(l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. @return \)\Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double GammaHlljjRatio() const; /** @brief The new physics contribution to the ratio of the \)\Gamma(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) @return \)\delta \Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double deltaGammaHlljjRatio1() const; /** @brief The new physics contribution to the ratio of the \)\Gamma(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) @return \)\delta \Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double deltaGammaHlljjRatio2() const; /** @brief The ratio of the Br\)(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. @return Br\)(H\to l l j j) \(/Br\)(H\to l l j j)_{\mathrm{SM}} \( */ virtual const double BrHlljjRatio() const; /** @brief The ratio of the \)\Gamma(H\to l \nu j j) \( (\)l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. More...
 
const double GammaHLvudRatio () const
 The ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
const double GammaHLvvLRatio () const
 The ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More...
 
const double GammaHmumuRatio () const
 The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. More...
 
const double GammaHssRatio () const
 The ratio of the \(\Gamma(H\to ss)\) in the current model and in the Standard Model. More...
 
const double GammaHtautauRatio () const
 The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. More...
 
const double GammaHudduRatio () const
 The ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. More...
 
const double GammaHWffRatio () const
 The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
const double GammaHWjjRatio () const
 The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. More...
 
const double GammaHWlvRatio () const
 The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
const double GammaHWW2l2vRatio () const
 The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
const double GammaHWW4fRatio () const
 The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
const double GammaHWW4jRatio () const
 The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. More...
 
const double GammaHWWRatio () const
 The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. More...
 
const double GammaHZddRatio () const
 The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
const double GammaHZeeRatio () const
 The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. More...
 
const double GammaHZffRatio () const
 The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
const double GammaHZgaRatio () const
 The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. More...
 
const double GammaHZllRatio () const
 The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
const double GammaHZmumuRatio () const
 The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. More...
 
const double GammaHZuuRatio () const
 The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
const double GammaHZvvRatio () const
 The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. More...
 
const double GammaHZZ2e2muRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. More...
 
const double GammaHZZ4dRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More...
 
const double GammaHZZ4eRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More...
 
const double GammaHZZ4fRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More...
 
const double GammaHZZ4lRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More...
 
const double GammaHZZ4muRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More...
 
const double GammaHZZ4uRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More...
 
const double GammaHZZ4vRatio () const
 The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More...
 
const double GammaHZZRatio () const
 The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. More...
 
virtual const double GammaW () const
 The total width of the \(W\) boson, \(\Gamma_W\). More...
 
virtual const double GammaW (const Particle fi, const Particle fj) const
 A partial decay width of the \(W\) boson decay into a SM fermion pair. More...
 
void GenerateSMInitialConditions ()
 Generates the initial condition for the Standard Model parameters. More...
 
double getCG_LNP () const
 Return CG_LNP. More...
 
const double getCW_tree () const
 
const double getDelta_ale () const
 
const double getDelta_g1 () const
 
const double getDelta_g2 () const
 
const double getDelta_Mz2 () const
 
const double getDelta_v () const
 
const double getDelta_xBZ () const
 
const double getDelta_xWZ () const
 
const double getEeMz () const
 
const double getG1_tree () const
 
const double getG2_tree () const
 
const double getG3_tree () const
 
const double getGZdL () const
 
const double getGZdR () const
 
const double getGZlL () const
 
const double getGZlR () const
 
const double getGZuL () const
 
const double getGZuR () const
 
const double getGZvL () const
 
double getLambda_NP () const
 Return Lambda_NP. More...
 
const double getLambdaH_tree () const
 
virtual NPSMEFTd6GeneralMatchinggetMatching () const
 A method to get the Matching object for this model. More...
 
std::array< double, 3 > getMd_LEW () const
 
std::array< double, 3 > getMe_LEW () const
 
std::array< double, 3 > getMu_LEW () const
 
const double getMw_tree () const
 
double getSMEFTCoeff (const std::string name, const double mu) const
 
double getSMEFTCoeff (const std::string name, int i, int j, const double mu) const
 
double getSMEFTCoeff (const std::string name, int i, int j, int k, int l, const double mu) const
 
double getSMEFTCoeffEW (const std::string name) const
 
double getSMEFTCoeffEW (const std::string name, int i, int j) const
 
double getSMEFTCoeffEW (const std::string name, int i, int j, int k, int l) const
 
gslpp::complex getSMEFTCoeffEWMB (const std::string name, int i, int j, gslpp::matrix< gslpp::complex > Vi, gslpp::matrix< gslpp::complex > Vj) const
 
gslpp::complex getSMEFTCoeffEWMB (const std::string name, int i, int j, int k, int l, gslpp::matrix< gslpp::complex > Vi, gslpp::matrix< gslpp::complex > Vj, gslpp::matrix< gslpp::complex > Vk, gslpp::matrix< gslpp::complex > Vl) const
 
gslpp::complex getSMEFTCoeffMB (const std::string name, int i, int j, gslpp::matrix< gslpp::complex > Vi, gslpp::matrix< gslpp::complex > Vj, const double mu) const
 
gslpp::complex getSMEFTCoeffMB (const std::string name, int i, int j, int k, int l, gslpp::matrix< gslpp::complex > Vi, gslpp::matrix< gslpp::complex > Vj, gslpp::matrix< gslpp::complex > Vk, gslpp::matrix< gslpp::complex > Vl, const double mu) const
 
const RGESolver & getSMEFTEvol () const
 
RGESolver getSMEFTEvolEW () const
 
const double getSW_tree () const
 
const gslpp::matrix< gslpp::complex > & getVdL () const
 
const gslpp::matrix< gslpp::complex > & getVdLd () const
 
const gslpp::matrix< gslpp::complex > & getVdR () const
 
const gslpp::matrix< gslpp::complex > & getVdRd () const
 
const gslpp::matrix< gslpp::complex > & getVeL () const
 
const gslpp::matrix< gslpp::complex > & getVeLd () const
 
const gslpp::matrix< gslpp::complex > & getVeR () const
 
const gslpp::matrix< gslpp::complex > & getVeRd () const
 
const gslpp::matrix< gslpp::complex > & getVuL () const
 
const gslpp::matrix< gslpp::complex > & getVuLd () const
 
const gslpp::matrix< gslpp::complex > & getVuR () const
 
const gslpp::matrix< gslpp::complex > & getVuRd () const
 
const double getXBZ_tree () const
 
const double getXWZ_tree () const
 
gslpp::matrix< gslpp::complex > getYd () const
 
gslpp::matrix< gslpp::complex > getYe () const
 
gslpp::matrix< gslpp::complex > getYu () const
 
virtual const double IctW_TWG (const double mu) const
 
virtual const double IctZ_TWG (const double mu) const
 
virtual const double intDMLL2eus2 (const double s, const double t0, const double t1) const
 
virtual const double intDMLR2etildest2 (const double s, const double t0, const double t1) const
 
virtual const double intDMLR2ets2 (const double s, const double t0, const double t1) const
 
virtual const double intDMRL2etildest2 (const double s, const double t0, const double t1) const
 
virtual const double intDMRL2ets2 (const double s, const double t0, const double t1) const
 
virtual const double intDMRR2eus2 (const double s, const double t0, const double t1) const
 
virtual const double kappaAeff () const
 The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\). More...
 
virtual const double kappabeff () const
 The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\). More...
 
virtual const double kappaceff () const
 The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\). More...
 
virtual const double kappaGeff () const
 The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\). More...
 
virtual const double kappamueff () const
 The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\). More...
 
virtual const double kappaseff () const
 The effective coupling \(\kappa_{s,eff}=\sqrt{\Gamma_{Hss}/\Gamma_{Hss}^{SM}}\). More...
 
virtual const double kappataueff () const
 The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\). More...
 
virtual const double kappaW4feff () const
 The effective coupling \(\kappa_{W4f,eff}=\sqrt{\Gamma_{H4f, CC}/\Gamma_{H4f, CC}^{SM}}\). More...
 
virtual const double kappaWeff () const
 The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\). More...
 
virtual const double kappaZ4feff () const
 The effective coupling \(\kappa_{Z4f,eff}=\sqrt{\Gamma_{H4f, NC}/\Gamma_{H4f, NC}^{SM}}\). More...
 
virtual const double kappaZAeff () const
 The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\). More...
 
virtual const double kappaZeff () const
 The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\). More...
 
virtual const double lambdaZNP (const double mu) const
 The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\). More...
 
virtual const double lambz_HB (const double mu) const
 The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More...
 
virtual const double mubbH (const double sqrt_s) const
 The ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model. More...
 
virtual const double mueeHee (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{e^+e^- \to He^+e^-}\) between the \( e^+e^- \to H e^+e^- \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double mueeHvv (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double mueettH (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual const double mueeWBF (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual const double mueeWW (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More...
 
virtual const double mueeZBF (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More...
 
virtual const double mueeZH (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double mueeZHGen (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double mueeZHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double mueeZllH (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double mueeZllHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double mueeZqqH (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double mueeZqqHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const
 The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double muepWBF (const double sqrt_s) const
 The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model. More...
 
virtual const double muepZBF (const double sqrt_s) const
 The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model. More...
 
virtual const double muggH (const double sqrt_s) const
 The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More...
 
virtual const double muggHbb (const double sqrt_s) const
 The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual const double muggHgaga (const double sqrt_s) const
 The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual const double muggHH (const double sqrt_s) const
 The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].) More...
 
virtual const double muggHmumu (const double sqrt_s) const
 The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual const double muggHpttH (const double sqrt_s) const
 The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double muggHtautau (const double sqrt_s) const
 The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual const double muggHWW (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual const double muggHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual const double muggHZga (const double sqrt_s) const
 The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual const double muggHZZ (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual const double muggHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual const double mummH (const double sqrt_s) const
 The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model. More...
 
virtual const double mummHmm (const double sqrt_s) const
 The ratio \(\mu_{\mu\mu H\mu\mu}\) between the \(\sigma(\mu \mu \to H \mu \mu)}\) production cross-section in the current model and in the Standard Model. More...
 
virtual const double mummHNWA (const double sqrt_s) const
 The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model, in the narrow width approximation. More...
 
virtual const double mummHvv (const double sqrt_s) const
 The ratio \(\mu_{\mu\mu H\nu\nu}\) between the \(\sigma(\mu \mu \to H \nu \nu)}\) production cross-section in the current model and in the Standard Model. More...
 
virtual const double mummttH (const double sqrt_s) const
 The ratio \(\mu_{\mu\mu ttH}\) between the \(\sigma(\mu \mu \to t\bar{t} H )}\) production cross-section in the current model and in the Standard Model. More...
 
virtual const double mummZH (const double sqrt_s) const
 The ratio \(\mu_{\mu\mu ZH}\) between the \(\sigma(\mu \mu \to Z H)}\) production cross-section in the current model and in the Standard Model. More...
 
virtual const double mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const
 The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6General class. More...
 
virtual const double mutH (const double sqrt_s) const
 The ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double mutHq (const double sqrt_s) const
 The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double muTHUggHbb (const double sqrt_s) const
 The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual const double muTHUggHgaga (const double sqrt_s) const
 The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual const double muTHUggHmumu (const double sqrt_s) const
 The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUggHtautau (const double sqrt_s) const
 The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual const double muTHUggHWW (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual const double muTHUggHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUggHZga (const double sqrt_s) const
 The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual const double muTHUggHZgamumu (const double sqrt_s) const
 The ratio \(\mu_{ggH,Z\gamma\to \gamma 2\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\to \gamma 2\mu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUggHZZ (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual const double muTHUggHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual const double muTHUggHZZ4mu (const double sqrt_s) const
 The ratio \(\mu_{ggH,ZZ\to 4\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4\mu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUttHbb (const double sqrt_s) const
 The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual const double muTHUttHgaga (const double sqrt_s) const
 The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual const double muTHUttHmumu (const double sqrt_s) const
 The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUttHtautau (const double sqrt_s) const
 The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual const double muTHUttHWW (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual const double muTHUttHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUttHZga (const double sqrt_s) const
 The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual const double muTHUttHZZ (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual const double muTHUttHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVBFBRinv (const double sqrt_s) const
 The ratio \(\mu_{VBF}\) between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More...
 
virtual const double muTHUVBFHbb (const double sqrt_s) const
 The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVBFHgaga (const double sqrt_s) const
 The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual const double muTHUVBFHinv (const double sqrt_s) const
 The ratio \(\mu_{VBF,inv}\) between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More...
 
virtual const double muTHUVBFHmumu (const double sqrt_s) const
 The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVBFHtautau (const double sqrt_s) const
 The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVBFHWW (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVBFHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVBFHZga (const double sqrt_s) const
 The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVBFHZZ (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVBFHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVHbb (const double sqrt_s) const
 The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVHBRinv (const double sqrt_s) const
 The ratio \(\mu_{VH}\) between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More...
 
virtual const double muTHUVHgaga (const double sqrt_s) const
 The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual const double muTHUVHinv (const double sqrt_s) const
 The ratio \(\mu_{VH,inv}\) between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More...
 
virtual const double muTHUVHmumu (const double sqrt_s) const
 The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVHtautau (const double sqrt_s) const
 The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVHWW (const double sqrt_s) const
 The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVHZga (const double sqrt_s) const
 The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVHZZ (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual const double muTHUVHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual const double muTHUWHbb (const double sqrt_s) const
 The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual const double muTHUWHgaga (const double sqrt_s) const
 The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual const double muTHUWHmumu (const double sqrt_s) const
 The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUWHtautau (const double sqrt_s) const
 The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual const double muTHUWHWW (const double sqrt_s) const
 The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual const double muTHUWHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUWHZga (const double sqrt_s) const
 The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual const double muTHUWHZZ (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual const double muTHUWHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual const double muTHUZHbb (const double sqrt_s) const
 The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual const double muTHUZHgaga (const double sqrt_s) const
 The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual const double muTHUZHmumu (const double sqrt_s) const
 The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUZHtautau (const double sqrt_s) const
 The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual const double muTHUZHWW (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual const double muTHUZHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual const double muTHUZHZga (const double sqrt_s) const
 The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual const double muTHUZHZZ (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual const double muTHUZHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual const double muttH (const double sqrt_s) const
 The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double muttHbb (const double sqrt_s) const
 The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual const double muttHgaga (const double sqrt_s) const
 The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual const double muttHgagaZeeboost (const double sqrt_s) const
 The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H\to b\bar{b}\), \(Z\to e^+e^-\) channel channel in the current model and in the Standard Model. More...
 
virtual const double muttHmumu (const double sqrt_s) const
 The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual const double muttHtautau (const double sqrt_s) const
 The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual const double muttHWW (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual const double muttHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual const double muttHZbbboost (const double sqrt_s) const
 The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model. More...
 
virtual const double muttHZga (const double sqrt_s) const
 The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual const double muttHZZ (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual const double muttHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual const double muVBF (const double sqrt_s) const
 The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More...
 
virtual const double muVBFgamma (const double sqrt_s) const
 The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model. More...
 
virtual const double muVBFHbb (const double sqrt_s) const
 The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual const double muVBFHgaga (const double sqrt_s) const
 The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual const double muVBFHmumu (const double sqrt_s) const
 The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual const double muVBFHtautau (const double sqrt_s) const
 The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual const double muVBFHWW (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual const double muVBFHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual const double muVBFHZga (const double sqrt_s) const
 The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual const double muVBFHZZ (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual const double muVBFHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual const double muVBFpVH (const double sqrt_s) const
 The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double muVH (const double sqrt_s) const
 The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double muVHbb (const double sqrt_s) const
 The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual const double muVHgaga (const double sqrt_s) const
 The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual const double muVHmumu (const double sqrt_s) const
 The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual const double muVHpT250 (const double sqrt_s) const
 The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV. More...
 
virtual const double muVHtautau (const double sqrt_s) const
 The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual const double muVHWW (const double sqrt_s) const
 The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual const double muVHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual const double muVHZga (const double sqrt_s) const
 The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual const double muVHZZ (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual const double muVHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual const double muWH (const double sqrt_s) const
 The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double muWHbb (const double sqrt_s) const
 The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual const double muWHgaga (const double sqrt_s) const
 The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual const double muWHmumu (const double sqrt_s) const
 The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual const double muWHpT250 (const double sqrt_s) const
 The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV. More...
 
virtual const double muWHtautau (const double sqrt_s) const
 The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual const double muWHWW (const double sqrt_s) const
 The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual const double muWHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual const double muWHZga (const double sqrt_s) const
 The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual const double muWHZZ (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual const double muWHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual const double muZH (const double sqrt_s) const
 The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More...
 
virtual const double muZHbb (const double sqrt_s) const
 The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More...
 
virtual const double muZHgaga (const double sqrt_s) const
 The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More...
 
virtual const double muZHmumu (const double sqrt_s) const
 The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More...
 
virtual const double muZHpT250 (const double sqrt_s) const
 The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV. More...
 
virtual const double muZHtautau (const double sqrt_s) const
 The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More...
 
virtual const double muZHWW (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More...
 
virtual const double muZHWW2l2v (const double sqrt_s) const
 The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More...
 
virtual const double muZHZga (const double sqrt_s) const
 The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More...
 
virtual const double muZHZZ (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More...
 
virtual const double muZHZZ4l (const double sqrt_s) const
 The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More...
 
virtual const double Mw () const
 The mass of the \(W\) boson, \(M_W\). More...
 
virtual const double NevLHCppee13 (const int i_bin) const
 Number of di-electron events at the LHC at 13 TeV. More...
 
virtual const double NevLHCppenu13 (const int i_bin) const
 Number of mono-electron events at the LHC at 13 TeV. More...
 
virtual const double NevLHCppmumu13 (const int i_bin) const
 Number of di-muon events at the LHC at 13 TeV. More...
 
virtual const double NevLHCppmunu13 (const int i_bin) const
 Number of mono-muon events at the LHC at 13 TeV. More...
 
virtual const double NevLHCpptaunu13 (const int i_bin) const
 Number of mono-tau events at the LHC at 13 TeV. More...
 
virtual const double NevLHCpptautau13 (const int i_bin) const
 Number of di-tau events at the LHC at 13 TeV. More...
 
 NPSMEFTd6General ()
 Constructor. More...
 
virtual const double obliqueS () const
 The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).) More...
 
virtual const double obliqueT () const
 The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).) More...
 
virtual const double obliqueU () const
 The oblique parameter \(U\). More...
 
virtual const double obliqueW () const
 The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).) More...
 
virtual const double obliqueY () const
 The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).) More...
 
virtual const double ppZHprobe (const double sqrt_s) const
 The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6General class. More...
 
virtual bool PreUpdate ()
 The pre-update method for NPSMEFTd6General. More...
 
void printNonVanishingSMEFTCoeffEW () const
 
virtual const double R0_f (const Particle f) const
 The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More...
 
virtual const double RWc () const
 The ratio \(R_{W,c)=\Gamma(W\to c + X)/\Gamma(W\to had)\). More...
 
virtual const double RWlilj (const Particle li, const Particle lj) const
 The lepton universality ratio \(R_{W,l_i/l_j)=\Gamma(W\to l_i \nu_i)/\Gamma(W\to l_j \nu_j)\). More...
 
virtual const double RZlilj (const Particle li, const Particle lj) const
 The lepton universality ratio \(R_{Z,l_i/l_j)=\Gamma(Z\to l_i^+ l_i^-)/\Gamma(Z\to l_j^+ l_j^-)\). More...
 
virtual bool setFlag (const std::string name, const bool value)
 A method to check if all the mandatory parameters for NPSMEFTd6General have been provided in model initialization. More...
 
virtual bool setFlagStr (const std::string name, const std::string value)
 A method to set a flag of NPSMEFTd6General. More...
 
virtual const double sigma0_had () const
 The cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\sigma_h^0\). More...
 
virtual const double STXS0_qqH (const double sqrt_s) const
 The STXS0 bin \(pp \to H qq\). More...
 
virtual const double STXS12_BrH4lRatio () const
 The STXS BR \( H \to 4l \), \(l=e,\mu\). More...
 
virtual const double STXS12_BrHbbRatio () const
 The STXS BR \( H \to bb \). More...
 
virtual const double STXS12_BrHevmuvRatio () const
 The STXS BR \( H \to e\nu \mu\nu \). More...
 
virtual const double STXS12_BrHgagaRatio () const
 The STXS BR \( H \to \gamma \gamma \). More...
 
virtual const double STXS12_ggH_mjj0_350_pTH0_60_Nj1 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j \geq 1,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60\). More...
 
virtual const double STXS12_ggH_mjj0_350_pTH0_60_Nj2 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60\). More...
 
virtual const double STXS12_ggH_mjj0_350_pTH120_200_Nj2 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~120<p_{TH} [GeV]<200\). More...
 
virtual const double STXS12_ggH_mjj0_350_pTH60_120_Nj2 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~60<p_{TH} [GeV]<120\). More...
 
virtual const double STXS12_ggH_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~<p_{TH} [GeV]<200\). More...
 
virtual const double STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\). More...
 
virtual const double STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\). More...
 
virtual const double STXS12_ggH_mjj700_Inf_pTH0_200_Nj2 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200\). More...
 
virtual const double STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\). More...
 
virtual const double STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\). More...
 
virtual const double STXS12_ggH_pTH0_10_Nj0 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j=0,~p_{TH} [GeV]<10\). More...
 
virtual const double STXS12_ggH_pTH0_60_Nj1 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j = 1,~p_{TH} [GeV]<60\). More...
 
virtual const double STXS12_ggH_pTH10_200_Nj0 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j=0,~p_{TH} [GeV]<10\). More...
 
virtual const double STXS12_ggH_pTH10_Inf_Nj0 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j=0,~10<p_{TH} [GeV]\). More...
 
virtual const double STXS12_ggH_pTH120_200_Nj1 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j = 1,~120<p_{TH} [GeV]<200\). More...
 
virtual const double STXS12_ggH_pTH200_300 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(,200<~p_{TH} [GeV]<300\). More...
 
virtual const double STXS12_ggH_pTH200_300_Nj01 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j\leq 1,~200<p_{TH} [GeV]<300\). More...
 
virtual const double STXS12_ggH_pTH300_450 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(,300<~p_{TH} [GeV]<450\). More...
 
virtual const double STXS12_ggH_pTH300_450_Nj01 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j\leq 1,~300<p_{TH} [GeV]<450\). More...
 
virtual const double STXS12_ggH_pTH450_650 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(450<~p_{TH} [GeV]<650\). More...
 
virtual const double STXS12_ggH_pTH450_650_Nj01 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j\leq 1,~450<p_{TH} [GeV]<650\). More...
 
virtual const double STXS12_ggH_pTH450_Inf (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(,450<~p_{TH} [GeV]\). More...
 
virtual const double STXS12_ggH_pTH60_120_Nj1 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j = 1,~60<p_{TH} [GeV]<120\). More...
 
virtual const double STXS12_ggH_pTH650_Inf (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(~p_{TH} [GeV]>650\). More...
 
virtual const double STXS12_ggH_pTH650_Inf_Nj01 (const double sqrt_s) const
 The STXS bin \(gg \to H\), \(N_j\leq 1,650<p_{TH} [GeV]\). More...
 
virtual const double STXS12_ggHll_pTV0_75 (const double sqrt_s) const
 The STXS bin \(gg \to H\ell\ell\), \(p_{TV}[GeV]<75\). More...
 
virtual const double STXS12_ggHll_pTV150_250_Nj0 (const double sqrt_s) const
 The STXS bin \(gg \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More...
 
virtual const double STXS12_ggHll_pTV150_250_Nj1 (const double sqrt_s) const
 The STXS bin \(gg \to H\ell\ell\), \(N_j = 1,~150<p_{TV}[GeV]<250\). More...
 
virtual const double STXS12_ggHll_pTV250_Inf (const double sqrt_s) const
 The STXS bin \(gg \to H\ell\ell\), \(250 < p_{TV}[GeV]\). More...
 
virtual const double STXS12_ggHll_pTV75_150 (const double sqrt_s) const
 The STXS bin \(gg \to H\ell\ell\), \(75<p_{TV}[GeV]<150\). More...
 
virtual const double STXS12_qqHll_pTV0_150 (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\ell\), \(0<p_{TV}<150[GeV]\). More...
 
virtual const double STXS12_qqHll_pTV0_75 (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\ell\), \(p_{TV}[GeV]<75\). More...
 
virtual const double STXS12_qqHll_pTV150_250_Nj0 (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More...
 
virtual const double STXS12_qqHll_pTV150_250_Nj1 (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\ell\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\). More...
 
virtual const double STXS12_qqHll_pTV250_400 (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}<400[GeV]\). More...
 
virtual const double STXS12_qqHll_pTV250_Inf (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}[GeV]\). More...
 
virtual const double STXS12_qqHll_pTV400_Inf (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\ell\), \(400<p_{TV}[GeV]\). More...
 
virtual const double STXS12_qqHll_pTV75_150 (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\ell\), \(75<p_{TV}[GeV]<150\). More...
 
virtual const double STXS12_qqHlv_pTV0_150 (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\nu\), \(0<p_{TV}<150[GeV]\). More...
 
virtual const double STXS12_qqHlv_pTV0_75 (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\nu\), \(p_{TV}[GeV]<75\). More...
 
virtual const double STXS12_qqHlv_pTV150_250_Nj0 (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\nu\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More...
 
virtual const double STXS12_qqHlv_pTV150_250_Nj1 (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\nu\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\). More...
 
virtual const double STXS12_qqHlv_pTV250_400 (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}<400[GeV]\). More...
 
virtual const double STXS12_qqHlv_pTV250_Inf (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}[GeV]\). More...
 
virtual const double STXS12_qqHlv_pTV400_Inf (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\nu\), \(400<p_{TV}[GeV]\). More...
 
virtual const double STXS12_qqHlv_pTV75_150 (const double sqrt_s) const
 The STXS bin \(qq \to H\ell\nu\), \(75<p_{TV}[GeV]<150\). More...
 
virtual const double STXS12_qqHqq_mjj0_60_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~m_{jj}[GeV]<60\). More...
 
virtual const double STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1000<m_{jj}[GeV]<1500,~p_{TH}[GeV]<200\). More...
 
virtual const double STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1000<m_{jj}[GeV],~p_{TH}[GeV]>200\). More...
 
virtual const double STXS12_qqHqq_mjj120_350_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~120<m_{jj}[GeV]<350\). More...
 
virtual const double STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1500<m_{jj}[GeV],~p_{TH}[GeV]<200\). More...
 
virtual const double STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<1000,~p_{TH}[GeV]>200\). More...
 
virtual const double STXS12_qqHqq_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200\). More...
 
virtual const double STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\). More...
 
virtual const double STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\). More...
 
virtual const double STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV],~200<p_{TH}[GeV]\). More...
 
virtual const double STXS12_qqHqq_mjj60_120_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~60<m_{jj}[GeV]<120\). More...
 
virtual const double STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV]<1000,~p_{TH}[GeV]<200\). More...
 
virtual const double STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\). More...
 
virtual const double STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\). More...
 
virtual const double STXS12_qqHqq_Nj0 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j = 0\). More...
 
virtual const double STXS12_qqHqq_Nj1 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j = 1\). More...
 
virtual const double STXS12_qqHqq_VH_veto_Nj01 (const double sqrt_s) const
 The STXS bin \(qq \to Hqq\), \(N_j = 0,1\) VH-veto Ref. 2402.05742. More...
 
virtual const double STXS12_tH (const double sqrt_s) const
 The STXS bin \(pp \to tH\). More...
 
virtual const double STXS12_ttH_pTH0_60 (const double sqrt_s) const
 The STXS bin \(pp \to ttH\), \(p_{TH}[GeV]<60\). More...
 
virtual const double STXS12_ttH_pTH120_200 (const double sqrt_s) const
 The STXS bin \(pp \to ttH\), \(120<p_{TH}[GeV]<200\). More...
 
virtual const double STXS12_ttH_pTH200_300 (const double sqrt_s) const
 The STXS bin \(pp \to ttH\), \(200<p_{TH}[GeV]<300\). More...
 
virtual const double STXS12_ttH_pTH300_450 (const double sqrt_s) const
 The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]<450\). More...
 
virtual const double STXS12_ttH_pTH300_Inf (const double sqrt_s) const
 The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]\). More...
 
virtual const double STXS12_ttH_pTH450_Inf (const double sqrt_s) const
 The STXS bin \(pp \to ttH\), \(450<p_{TH}[GeV]\). More...
 
virtual const double STXS12_ttH_pTH60_120 (const double sqrt_s) const
 The STXS bin \(pp \to ttH\), \(60<p_{TH}[GeV]<120\). More...
 
virtual const double STXS_ggH0j (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual const double STXS_ggH1j_pTH_0_60 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual const double STXS_ggH1j_pTH_120_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual const double STXS_ggH1j_pTH_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual const double STXS_ggH1j_pTH_60_120 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual const double STXS_ggH2j_pTH_0_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual const double STXS_ggH2j_pTH_0_60 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual const double STXS_ggH2j_pTH_120_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual const double STXS_ggH2j_pTH_200 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual const double STXS_ggH2j_pTH_60_120 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual const double STXS_ggH_VBFtopo_j3 (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual const double STXS_ggH_VBFtopo_j3v (const double sqrt_s) const
 The STXS bin \(gg \to H\). More...
 
virtual const double STXS_qqHll_pTV_0_150 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual const double STXS_qqHll_pTV_150_250 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual const double STXS_qqHll_pTV_150_250_0j (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual const double STXS_qqHll_pTV_150_250_1j (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual const double STXS_qqHll_pTV_250 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \ell\). More...
 
virtual const double STXS_qqHlv_pTV_0_150 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual const double STXS_qqHlv_pTV_0_250 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual const double STXS_qqHlv_pTV_150_250_0j (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual const double STXS_qqHlv_pTV_150_250_1j (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual const double STXS_qqHlv_pTV_250 (const double sqrt_s) const
 The STXS bin \(qq \to H \ell \nu\). More...
 
virtual const double STXS_qqHqq_nonVHtopo (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual const double STXS_qqHqq_pTj_200 (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual const double STXS_qqHqq_Rest (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual const double STXS_qqHqq_VBFtopo_j3 (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual const double STXS_qqHqq_VBFtopo_j3v (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual const double STXS_qqHqq_VBFtopo_Rest (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual const double STXS_qqHqq_VHtopo (const double sqrt_s) const
 The STXS bin \(qq \to H qq\). More...
 
virtual const double STXS_ttHtH (const double sqrt_s) const
 The STXS bin \( ttH + tH \). More...
 
virtual const double STXS_WHqqHqq_pTj1_200 (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual const double STXS_WHqqHqq_Rest (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual const double STXS_WHqqHqq_VBFtopo_j3 (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual const double STXS_WHqqHqq_VBFtopo_j3v (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual const double STXS_WHqqHqq_VH2j (const double sqrt_s) const
 The STXS bin \( qq \to WH \to H qq \). More...
 
virtual const double STXS_ZHqqHqq_pTj1_200 (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual const double STXS_ZHqqHqq_Rest (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual const double STXS_ZHqqHqq_VBFtopo_j3 (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual const double STXS_ZHqqHqq_VBFtopo_j3v (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
virtual const double STXS_ZHqqHqq_VH2j (const double sqrt_s) const
 The STXS bin \( qq \to ZH \to H qq \). More...
 
const double tovers2 (const double cosmin, const double cosmax) const
 
const double uovers2 (const double cosmin, const double cosmax) const
 
double xlog1 (const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const
 
double xlog2 (const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const
 
double xlog3 (const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const
 
double xlog4 (const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const
 
double xlog5 (const double C1Lambda, const double C2, const double C3, const double C4, const double C5, const double C6muw) const
 
virtual const double xseeWW (const double sqrt_s) const
 Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\). More...
 
virtual const double xseeWW4fLEP2 (const double sqrt_s, const int fstate) const
 The cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More...
 
virtual const double xseeWWtotLEP2 (const double sqrt_s) const
 The total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More...
 
- Public Member Functions inherited from NPbase
virtual const double alrmoller (const double q2, const double y) const
 
virtual const double amuon () const
 
virtual const double BR_Zf (const Particle f) const
 The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\). More...
 
virtual const double BrHlljjRatio () const
 The ratio of the Br \((H\to l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More...
 
virtual const double C1eeHvv (const double sqrt_s) const
 The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...
 
virtual const double C1eettH (const double sqrt_s) const
 The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...
 
virtual const double C1eeWBF (const double sqrt_s) const
 The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...
 
virtual const double C1eeZBF (const double sqrt_s) const
 The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...
 
virtual const double C1eeZH (const double sqrt_s) const
 The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More...
 
const double C1Htot () const
 The C1 coefficient controlling the H^3 corrections to the total Higgs width from the Higgs trilinear coupling. More...
 
virtual const double cbminuscc () const
 
virtual const double cbminusctau () const
 
virtual const double ccminusctau () const
 
virtual const double cgaplusct () const
 
virtual const double cgminuscga () const
 
virtual const double cgplusct () const
 
virtual const double cVpluscb () const
 
virtual const double cVplusctau () const
 
virtual const double deltaA_f_2 (const Particle f) const
 The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\Delta \mathcal{A}_f^{(2)}\). More...
 
virtual const double deltaAFB_2 (const Particle f) const
 The \(\mathcal{O}(\Lambda^{-4})\) new physics to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\Delta A^f_{FB}\). More...
 
virtual const double deltaGA_f_2 (const Particle f) const
 
virtual const double deltaGamma_Z_2 () const
 The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the total decay width of the \(Z\) boson, \(\Delta \Gamma_Z^{(2)}\). More...
 
virtual const double deltaGamma_Zf_2 (const Particle f) const
 The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\Delta \Gamma_{Z,f}^{(2)}\). More...
 
virtual const double deltaGamma_Zhad () const
 The new physics contribution to the hadronic decay width of the \(Z\) boson, \(\delta \Gamma_{Z,had}\). More...
 
virtual const double deltaGamma_Zhad_2 () const
 The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the hadronic decay width of the \(Z\) boson, \(\Delta \Gamma_{Z,had}^{(2)}\). More...
 
const double deltaGL_f_mu (const Particle p, const double mu) const
 New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More...
 
const double deltaGR_f_mu (const Particle p, const double mu) const
 New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More...
 
virtual const double deltaGV_f_2 (const Particle f) const
 
virtual const double deltaN_nu () const
 The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements. More...
 
virtual const double deltaR0_f_2 (const Particle f) const
 The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos: More...
 
virtual const double deltaR_inv () const
 The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the \(Z\) boson, \(\delta R_{inv}\). More...
 
virtual const double deltaRuc () const
 The new physics contribution to the ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width: More...
 
virtual const double deltaRuc_2 () const
 The \(\mathcal{O}(1/\Lambda^4)\) new physics contribution to the ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width: More...
 
virtual const double deltaSigmaHadron_2 () const
 The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\Delta \sigma_h^{0,(2)}\). More...
 
virtual const double deltaSin2thetaEff_e () const
 The new physics contribution to the effective electron/leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. More...
 
virtual const double deltaSin2thetaEff_e_2 () const
 The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the effective electron weak angle \(\Delta \sin^2\theta_{eff,e}^{(2)}\) at the \(Z\) pole. More...
 
virtual const double deltaSin2thetaEff_mu () const
 The new physics contribution to the effective muonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\mu\mu}\) at the \(Z\) pole. More...
 
virtual const double deltaSin2thetaEff_mu_2 () const
 The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the effective muonic weak angle \(\Delta \sin^2\theta_{eff, \mu}^{(2)}\) at the \(Z\) pole. More...
 
virtual const double deltaxseeWWhadLEP2 (const double sqrt_s) const
 The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to j j j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...
 
virtual const double deltaxseeWWleptLEP2 (const double sqrt_s) const
 The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...
 
virtual const double deltaxseeWWsemilLEP2 (const double sqrt_s) const
 The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...
 
virtual const double eeffAFBbottom (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffAFBcharm (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffAFBe (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffAFBetsub (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffAFBmu (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffAFBstrange (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffAFBtau (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffRbottom (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffRcharm (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffRelectron (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffRelectrontsub (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffRmuon (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffRstrange (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffRtau (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffsigma (const Particle f, const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const
 
virtual const double eeffsigmaBottom (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffsigmaCharm (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffsigmaE (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffsigmaEtsub (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffsigmaHadron (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffsigmaMu (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffsigmaStrange (const double pol_e, const double pol_p, const double s) const
 
virtual const double eeffsigmaTau (const double pol_e, const double pol_p, const double s) const
 
virtual const gslpp::complex gA_f (const Particle f) const
 The total (SM+NP) contribution to the neutral-current axial-vector coupling \(g_A^f\). More...
 
virtual const double Gamma_had () const
 The hadronic decay width of the \(Z\) boson, \(\Gamma_{Z,had}\). More...
 
virtual const double gAnue () const
 
virtual const StandardModelgetTrueSM () const
 A method to return a StandardModel object from NPbase. More...
 
virtual const double gLnuN2 () const
 
virtual const double gRnuN2 () const
 
virtual const gslpp::complex gV_f (const Particle f) const
 The total (SM+NP) contribution to the neutral-current vector coupling \(g_V^f\). More...
 
virtual const double gVnue () const
 
virtual const gslpp::complex kappaZ_f (const Particle f) const
 The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions. More...
 
virtual const double LEP2AFBbottom (const double s) const
 
virtual const double LEP2AFBcharm (const double s) const
 
virtual const double LEP2AFBe (const double s) const
 
virtual const double LEP2AFBmu (const double s) const
 
virtual const double LEP2AFBtau (const double s) const
 
virtual const double LEP2dsigmadcosBinE (const double s, const double cos, const double cosmin, const double cosmax) const
 
virtual const double LEP2dsigmadcosBinMu (const double s, const double cos, const double cosmin, const double cosmax) const
 
virtual const double LEP2dsigmadcosBinTau (const double s, const double cos, const double cosmin, const double cosmax) const
 
virtual const double LEP2dsigmadcosE (const double s, const double cos) const
 
virtual const double LEP2dsigmadcosMu (const double s, const double cos) const
 
virtual const double LEP2dsigmadcosTau (const double s, const double cos) const
 
virtual const double LEP2Rbottom (const double s) const
 
virtual const double LEP2Rcharm (const double s) const
 
virtual const double LEP2sigmaBottom (const double s) const
 
virtual const double LEP2sigmaCharm (const double s) const
 
virtual const double LEP2sigmaE (const double s) const
 
virtual const double LEP2sigmaHadron (const double s) const
 
virtual const double LEP2sigmaMu (const double s) const
 
virtual const double LEP2sigmaTau (const double s) const
 
virtual const double muggHgagaInt (const double sqrt_s) const
 The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259. More...
 
virtual const double muggHpbbH_Hgaga (const double sqrt_s) const
 
virtual const double muggHpbbH_Htautau (const double sqrt_s) const
 
virtual const double muggHpbbH_HWW (const double sqrt_s) const
 
virtual const double muggHpbbH_HZZ (const double sqrt_s) const
 
virtual const double muggHpttHptHpbbH_Hmumu (const double sqrt_s) const
 
virtual const double muggHpttHptHpbbH_HZga (const double sqrt_s) const
 
virtual const double muggHpVBFpbbH_Hbb (const double sqrt_s) const
 
virtual const double muppHmumu (const double sqrt_s) const
 
virtual const double muppHZga (const double sqrt_s) const
 
virtual const double mutHgaga (const double sqrt_s) const
 
virtual const double muttHptH_Hbb (const double sqrt_s) const
 
virtual const double muttHptH_Hgaga (const double sqrt_s) const
 
virtual const double muttHptH_Hmumu (const double sqrt_s) const
 
virtual const double muttHptH_Htautau (const double sqrt_s) const
 
virtual const double muttHptH_HWW (const double sqrt_s) const
 
virtual const double muttHptH_HZZ (const double sqrt_s) const
 
virtual const double muVBFpVH_Hmumu (const double sqrt_s) const
 
virtual const double muVBFpVH_HZga (const double sqrt_s) const
 
virtual const double muVHcc (const double sqrt_s) const
 
virtual const double N_nu () const
 The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\). More...
 
 NPbase ()
 The default constructor. More...
 
virtual int OutputOrder () const
 
virtual const double Qwemoller (const double q2, const double y) const
 
virtual const double Qwn () const
 
virtual const double Qwp () const
 
virtual const double R_inv () const
 The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\). More...
 
virtual const gslpp::complex rhoZ_f (const Particle f) const
 The effective neutral-current coupling \(\rho_Z^f\) including SM plus NP contributions. More...
 
virtual const double Ruc () const
 The ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width. More...
 
virtual const double sigmaSM_ee (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const
 
virtual const double sin2thetaEff (const Particle f) const
 The leptonic effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\rm lept}\) at the the \(Z\) pole. More...
 
virtual const double TauLFU_gmuge () const
 
virtual const double TauLFU_gtauge () const
 
virtual const double TauLFU_gtaugmu () const
 
virtual const double TauLFU_gtaugmuK () const
 
virtual const double TauLFU_gtaugmuPi () const
 
virtual bool Update (const std::map< std::string, double > &DPars)
 The update method for NPbase. More...
 
virtual const double UpperLimitZgammaA (const double sqrt_s) const
 
virtual const double UpperLimitZgammaA13 (const double sqrt_s) const
 
virtual const double UpperLimitZgammaC (const double sqrt_s) const
 
virtual const double UpperLimitZgammaC13 (const double sqrt_s) const
 
virtual const double xseeWWhadLEP2 (const double sqrt_s) const
 The cross section in pb for \(e^+ e^- \to W^+ W^- \to j j j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...
 
virtual const double xseeWWleptLEP2 (const double sqrt_s) const
 The cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...
 
virtual const double xseeWWsemilLEP2 (const double sqrt_s) const
 The cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More...
 
- Public Member Functions inherited from StandardModel
gslpp::complex AH_f (const double tau) const
 Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More...
 
gslpp::complex AH_W (const double tau) const
 W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling. More...
 
gslpp::complex AHZga_f (const double tau, const double lambda) const
 Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
gslpp::complex AHZga_W (const double tau, const double lambda) const
 W loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
const double Ale (double mu, orders order, bool Nf_thr=true) const
 The running electromagnetic coupling \(\alpha_e(\mu)\) in the \(\overline{MS}\) scheme. More...
 
const double ale_OS (const double mu, orders order=FULLNLO) const
 The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell scheme. More...
 
const double Als (const double mu, const int Nf_in, const orders order=FULLNLO) const
 Computes the running strong coupling \(\alpha_s(\mu)\) with \(N_f\) active flavours in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...
 
const double Als (const double mu, const orders order, const bool Nf_thr, const bool qed_flag) const
 The running QCD coupling \(\alpha(\mu)\) in the \(\overline{MS}\) scheme including QED corrections. More...
 
const double Als (const double mu, const orders order=FULLNLO, const bool Nf_thr=true) const
 
const double Alstilde5 (const double mu) const
 The value of \(\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\) and full EW corrections. More...
 
const double Beta_e (int nm, unsigned int nf) const
 QED beta function coefficients - eq. (36) hep-ph/0512066. More...
 
const double Beta_s (int nm, unsigned int nf) const
 QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066. More...
 
virtual const double BrHtobb () const
 The Br \((H\to b \bar{b})\) in the Standard Model. More...
 
virtual const double BrHtocc () const
 The Br \((H\to c \bar{c})\) in the Standard Model. More...
 
virtual const double BrHtogaga () const
 The Br \((H\to \gamma \gamma)\) in the Standard Model. More...
 
virtual const double BrHtogg () const
 The Br \(\(H\to gg)\) in the Standard Model. More...
 
virtual const double BrHtomumu () const
 The Br \((H\to \mu^+ \mu^-)\) in the Standard Model. More...
 
virtual const double BrHtoss () const
 The Br \((H\to s \bar{s})\) in the Standard Model. More...
 
virtual const double BrHtotautau () const
 The Br \((H\to \tau^+ \tau^-)\) in the Standard Model. More...
 
virtual const double BrHtoWWstar () const
 The Br \((H\to W W^*)\) in the Standard Model. More...
 
virtual const double BrHtoZga () const
 The Br \((H\to Z \gamma)\) in the Standard Model. More...
 
virtual const double BrHtoZZstar () const
 The Br \((H\to Z Z^*)\) in the Standard Model. More...
 
const double c02 () const
 The square of the cosine of the weak mixing angle \(c_0^2\) defined without weak radiative corrections. More...
 
virtual bool CheckFlags () const
 A method to check the sanity of the set of model flags. More...
 
virtual bool CheckParameters (const std::map< std::string, double > &DPars)
 A method to check if all the mandatory parameters for StandardModel have been provided in model initialization. More...
 
bool checkSMparamsForEWPO ()
 A method to check whether the parameters relevant to the EWPO are updated. More...
 
const double computeBrHto4f () const
 The Br \((H\to 4f)\) in the Standard Model. More...
 
const double computeBrHto4l2 () const
 The Br \((H\to 4l)\) \(l=e,\mu\) in the Standard Model. More...
 
const double computeBrHto4l3 () const
 The Br \((H\to 4l)\) \(l=e,\mu,\tau\) in the Standard Model. More...
 
const double computeBrHto4q () const
 The Br \((H\to 4q)\) in the Standard Model. More...
 
const double computeBrHto4v () const
 The Br \((H\to 4\nu)\) in the Standard Model. More...
 
const double computeBrHtobb () const
 The Br \((H\to bb)\) in the Standard Model. More...
 
const double computeBrHtocc () const
 The Br \((H\to cc)\) in the Standard Model. More...
 
const double computeBrHtoevmuv () const
 The Br \((H\to e \nu \mu \nu)\) in the Standard Model. More...
 
const double computeBrHtogaga () const
 The Br \((H\to\gamma\gamma)\) in the Standard Model. More...
 
const double computeBrHtogg () const
 The Br \((H\to gg)\) in the Standard Model. More...
 
const double computeBrHtollvv2 () const
 The Br \((H\to l^+ l^- \nu \nu)\) \(l=e,\mu\) in the Standard Model. More...
 
const double computeBrHtollvv3 () const
 The Br \((H\to l^+ l^- \nu \nu)\) \(l=e,\mu,\tau\) in the Standard Model. More...
 
const double computeBrHtomumu () const
 The Br \((H\to \mu\mu)\) in the Standard Model. More...
 
const double computeBrHtoss () const
 The Br \((H\to ss)\) in the Standard Model. More...
 
const double computeBrHtotautau () const
 The Br \((H\to \tau\tau)\) in the Standard Model. More...
 
const double computeBrHtoWW () const
 The Br \((H\to WW)\) in the Standard Model. More...
 
const double computeBrHtoZga () const
 The Br \((H\to Z\gamma)\) in the Standard Model. More...
 
const double computeBrHtoZZ () const
 The Br \((H\to ZZ)\) in the Standard Model. More...
 
void ComputeDeltaR_rem (const double Mw_i, double DeltaR_rem[orders_EW_size]) const
 A method to collect \(\Delta r_{\mathrm{rem}}\) computed via subclasses. More...
 
void ComputeDeltaRho (const double Mw_i, double DeltaRho[orders_EW_size]) const
 A method to collect \(\Delta\rho\) computed via subclasses. More...
 
const double computeGammaHgaga_tt () const
 The top loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
 
const double computeGammaHgaga_tW () const
 The mixed \(t-W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
 
const double computeGammaHgaga_WW () const
 The \(W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More...
 
const double computeGammaHgg_bb () const
 The bottom loop contribution to \(H\to gg\) in the Standard Model. More...
 
const double computeGammaHgg_tb () const
 The top-bottom interference contribution to \(H\to gg\) in the Standard Model. More...
 
const double computeGammaHgg_tt () const
 The top loop contribution to \(H\to gg\) in the Standard Model. More...
 
const double computeGammaHTotal () const
 The Higgs total width in the Standard Model. More...
 
const double computeGammaHZga_tt () const
 The top loop contribution to \(H\to Z\gamma\) in the Standard Model. More...
 
const double computeGammaHZga_tW () const
 The mixed \(t-W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. More...
 
const double computeGammaHZga_WW () const
 The \(W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. Currently it returns the value of tab 41 in ref. [Heinemeyer:2013tqa]. More...
 
const double computeSigmabbH (const double sqrt_s) const
 The bbH production cross section in the Standard Model. More...
 
const double computeSigmaggH (const double sqrt_s) const
 The ggH cross section in the Standard Model. More...
 
const double computeSigmaggH_bb (const double sqrt_s) const
 The square of the bottom-quark contribution to the ggH cross section in the Standard Model. More...
 
const double computeSigmaggH_tb (const double sqrt_s) const
 The top-bottom interference contribution to the ggH cross section in the Standard Model. More...
 
const double computeSigmaggH_tt (const double sqrt_s) const
 The square of the top-quark contribution to the ggH cross section in the Standard Model. More...
 
const double computeSigmatHq (const double sqrt_s) const
 The tHq production cross section in the Standard Model. More...
 
const double computeSigmattH (const double sqrt_s) const
 The ttH production cross section in the Standard Model. More...
 
const double computeSigmaVBF (const double sqrt_s) const
 The VBF cross section in the Standard Model. More...
 
const double computeSigmaWF (const double sqrt_s) const
 The W fusion contribution \(\sigma_{WF}\) to higgs-production cross section in the Standard Model. More...
 
const double computeSigmaWH (const double sqrt_s) const
 The WH production cross section in the Standard Model. More...
 
const double computeSigmaZF (const double sqrt_s) const
 The Z fusion contribution \(\sigma_{ZF}\) to higgs-production cross section in the Standard Model. More...
 
const double computeSigmaZH (const double sqrt_s) const
 The ZH production cross section in the Standard Model. More...
 
const double computeSigmaZWF (const double sqrt_s) const
 The Z W interference fusion contribution \(\sigma_{ZWF}\) to higgs-production cross section in the Standard Model. More...
 
virtual const double cW2 () const
 
virtual const double cW2 (const double Mw_i) const
 The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as \(c_W^2\). More...
 
virtual const double Dalpha5hMz () const
 The 5-quark contribution to the running of the em constant to the \(Z\) pole. \(\Delta\alpha_{had}^{(5)}(M_Z)\). More...
 
const double DeltaAlpha () const
 The total corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha(M_Z^2)\). More...
 
const double DeltaAlphaL5q () const
 The sum of the leptonic and the five-flavour hadronic corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha^{\ell+5q}(M_Z^2)\). More...
 
const double DeltaAlphaLepton (const double s) const
 Leptonic contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{lept}}(s)\). More...
 
const double DeltaAlphaTop (const double s) const
 Top-quark contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{top}}(s)\). More...
 
virtual const gslpp::complex deltaKappaZ_f (const Particle f) const
 Flavour non-universal vertex corrections to \(\kappa_Z^l\), denoted by \(\Delta\kappa_Z^l\). More...
 
virtual const double DeltaR () const
 The SM prediction for \(\Delta r\) derived from that for the \(W\) boson mass. More...
 
virtual const double DeltaRbar () const
 The SM prediction for \(\Delta \overline{r}\) derived from that for the \(W\)-boson mass. More...
 
virtual const gslpp::complex deltaRhoZ_f (const Particle f) const
 Flavour non-universal vertex corrections to \(\rho_Z^l\), denoted by \(\Delta\rho_Z^l\). More...
 
const double eeffsigmaEbin (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const
 
virtual const double epsilon1 () const
 The SM contribution to the epsilon parameter \(\varepsilon_1\). More...
 
virtual const double epsilon2 () const
 The SM contribution to the epsilon parameter \(\varepsilon_2\). More...
 
virtual const double epsilon3 () const
 The SM contribution to the epsilon parameter \(\varepsilon_3\). More...
 
virtual const double epsilonb () const
 The SM contribution to the epsilon parameter \(\varepsilon_b\). More...
 
gslpp::complex f_triangle (const double tau) const
 Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More...
 
gslpp::complex g_triangle (const double tau) const
 Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
virtual const double Gamma_inv () const
 The invisible partial decay width of the \(Z\) boson, \(\Gamma_{\mathrm{inv}}\). More...
 
virtual const double Gamma_muon () const
 The computation of the muon decay. More...
 
virtual const double Gamma_tau_l_nunu (const Particle l) const
 The computation of the leptonic tau decays. More...
 
virtual const double GammaHtobb () const
 The \(\Gamma(H\to b \bar{b})\) in the Standard Model. More...
 
virtual const double GammaHtocc () const
 The \(\Gamma(H\to c \bar{c})\) in the Standard Model. More...
 
virtual const double GammaHtogaga () const
 The \(\Gamma(H\to \gamma \gamma)\) in the Standard Model. More...
 
virtual const double GammaHtogg () const
 The \(\Gamma(H\to gg)\) in the Standard Model. More...
 
virtual const double GammaHtomumu () const
 The \(\Gamma(H\to \mu^+ \mu^-)\) in the Standard Model. More...
 
virtual const double GammaHtoss () const
 The \(\Gamma(H\to s \bar{s})\) in the Standard Model. More...
 
virtual const double GammaHTot () const
 The total Higgs width \(\Gamma(H)\) in the Standard Model. More...
 
virtual const double GammaHtotautau () const
 The \(\Gamma(H\to \tau^+ \tau^-)\) in the Standard Model. More...
 
virtual const double GammaHtoWWstar () const
 The \(\Gamma(H\to W W^*)\) in the Standard Model. More...
 
virtual const double GammaHtoZga () const
 The \(\Gamma(H\to Z \gamma)\) in the Standard Model. More...
 
virtual const double GammaHtoZZstar () const
 The \(\Gamma(H\to Z Z^*)\) in the Standard Model. More...
 
virtual const double GammaZ (const Particle f) const
 The \(Z\to \ell\bar{\ell}\) partial decay width, \(\Gamma_\ell\). More...
 
const double getAle () const
 A get method to retrieve the fine-structure constant \(\alpha\). More...
 
const double getAlsMz () const
 A get method to access the value of \(\alpha_s(M_Z)\). More...
 
virtual const double getCBd () const
 The ratio of the absolute value of the $B_d$ mixing amplitude over the Standard Model value. More...
 
virtual const double getCBs () const
 The ratio of the absolute value of the $B_s$ mixing amplitude over the Standard Model value. More...
 
virtual const double getCCC1 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual const double getCCC2 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual const double getCCC3 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual const double getCCC4 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual const double getCCC5 () const
 A virtual implementation for the RealWeakEFTCC class. More...
 
virtual const double getCDMK () const
 The ratio of the real part of the $K$ mixing amplitude over the Standard Model value. More...
 
virtual const double getCepsK () const
 The ratio of the imaginary part of the $K$ mixing amplitude over the Standard Model value. More...
 
const CKMgetCKM () const
 A get method to retrieve the member object of type CKM. More...
 
const double getDAle5Mz () const
 A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More...
 
const double getDelGammaWlv () const
 A get method to retrieve the theoretical uncertainty in \(\Gamma_W_{l\nu}\), denoted as \(\delta\,\Gamma_W_{l\nu}\). More...
 
const double getDelGammaWqq () const
 A get method to retrieve the theoretical uncertainty in \(\Gamma_W_{qq}\), denoted as \(\delta\,\Gamma_W_{qq}\). More...
 
const double getDelGammaZ () const
 A get method to retrieve the theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\). More...
 
const double getDelMw () const
 A get method to retrieve the theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\). More...
 
const double getDelR0b () const
 A get method to retrieve the theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More...
 
const double getDelR0c () const
 A get method to retrieve the theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More...
 
const double getDelR0l () const
 A get method to retrieve the theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More...
 
const double getDelSigma0H () const
 A get method to retrieve the theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\). More...
 
const double getDelSin2th_b () const
 A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More...
 
const double getDelSin2th_l () const
 A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More...
 
const double getDelSin2th_q () const
 A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More...
 
const std::string getFlagKappaZ () const
 A method to retrieve the model flag KappaZ. More...
 
const std::string getFlagMw () const
 A method to retrieve the model flag Mw. More...
 
const std::string getFlagRhoZ () const
 A method to retrieve the model flag RhoZ. More...
 
const FlavourgetFlavour () const
 
const double getGF () const
 A get method to retrieve the Fermi constant \(G_\mu\). More...
 
const int getIterationNo () const
 
const ParticlegetLeptons (const QCD::lepton p) const
 A get method to retrieve the member object of a lepton. More...
 
virtual const double getMHl () const
 A get method to retrieve the Higgs mass \(m_h\). More...
 
virtual const double getmq (const QCD::quark q, const double mu) const
 The MSbar running quark mass computed at NLO. More...
 
const double getMuw () const
 A get method to retrieve the matching scale \(\mu_W\) around the weak scale. More...
 
const double getMw () const
 A get method to access the input value of the mass of the \(W\) boson \(M_W\). More...
 
EWSMApproximateFormulaegetMyApproximateFormulae () const
 A get method to retrieve the member pointer of type EWSMApproximateFormulae. More...
 
EWSMcachegetMyEWSMcache () const
 A get method to retrieve the member pointer of type EWSMcache. More...
 
LeptonFlavourgetMyLeptonFlavour () const
 
EWSMOneLoopEWgetMyOneLoopEW () const
 A get method to retrieve the member pointer of type EWSMOneLoopEW,. More...
 
EWSMThreeLoopEWgetMyThreeLoopEW () const
 
EWSMThreeLoopEW2QCDgetMyThreeLoopEW2QCD () const
 
EWSMThreeLoopQCDgetMyThreeLoopQCD () const
 
EWSMTwoFermionsLEP2getMyTwoFermionsLEP2 () const
 A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More...
 
EWSMTwoLoopEWgetMyTwoLoopEW () const
 
EWSMTwoLoopQCDgetMyTwoLoopQCD () const
 
const double getMz () const
 A get method to access the mass of the \(Z\) boson \(M_Z\). More...
 
virtual const double getPhiBd () const
 Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More...
 
virtual const double getPhiBs () const
 Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More...
 
const gslpp::matrix< gslpp::complex > getUPMNS () const
 A get method to retrieve the object of the PMNS matrix. More...
 
const gslpp::matrix< gslpp::complex > getVCKM () const
 A get method to retrieve the CKM matrix. More...
 
const gslpp::matrix< gslpp::complex > & getYd () const
 A get method to retrieve the Yukawa matrix of the down-type quarks, \(Y_d\). More...
 
const gslpp::matrix< gslpp::complex > & getYe () const
 A get method to retrieve the Yukawa matrix of the charged leptons, \(Y_e\). More...
 
const gslpp::matrix< gslpp::complex > & getYn () const
 A get method to retrieve the Yukawa matrix of the neutrinos, \(Y_\nu\). More...
 
const gslpp::matrix< gslpp::complex > & getYu () const
 A get method to retrieve the Yukawa matrix of the up-type quarks, \(Y_u\). More...
 
gslpp::complex I_triangle_1 (const double tau, const double lambda) const
 Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
gslpp::complex I_triangle_2 (const double tau, const double lambda) const
 Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More...
 
virtual bool InitializeModel ()
 A method to initialize the model. More...
 
const double intMLL2eeeeus2 (const double s, const double t0, const double t1) const
 
const double intMLR2eeeets2 (const double s, const double t0, const double t1) const
 
const double intMLRtilde2eeeest2 (const double s, const double t0, const double t1) const
 
const double intMRR2eeeeus2 (const double s, const double t0, const double t1) const
 
const bool IsFlagNoApproximateGammaZ () const
 A method to retrieve the model flag NoApproximateGammaZ. More...
 
const bool IsFlagWithoutNonUniversalVC () const
 A method to retrieve the model flag WithoutNonUniversalVC. More...
 
const bool isSMSuccess () const
 A get method to retrieve the success status of the Standard Model update and matching. More...
 
const double MLL2eeff (const Particle f, const double s, const double t) const
 
const double MLR2eeff (const Particle f, const double s) const
 
const double MRL2eeff (const Particle f, const double s) const
 
const double MRR2eeff (const Particle f, const double s, const double t) const
 
const double Mw_tree () const
 The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). More...
 
const double MwbarFromMw (const double Mw) const
 A method to convert the \(W\)-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More...
 
const double MwFromMwbar (const double Mwbar) const
 A method to convert the \(W\)-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More...
 
double Mzbar () const
 The \(Z\)-boson mass \(\overline{M}_Z\) in the complex-pole/fixed-width scheme. More...
 
virtual const double rho_GammaW (const Particle fi, const Particle fj) const
 EW radiative corrections to the width of \(W \to f_i \bar{f}_j\), denoted as \(\rho^W_{ij}\). More...
 
const double s02 () const
 The square of the sine of the weak mixing angle \(s_0^2\) defined without weak radiative corrections. More...
 
void setCKM (const CKM &CKMMatrix)
 A set method to change the CKM matrix. More...
 
void setFlagCacheInStandardModel (bool FlagCacheInStandardModel)
 A set method to change the model flag CacheInStandardModel of StandardModel. More...
 
void setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ)
 
bool setFlagSigmaForAFB (const bool flagSigmaForAFB_i)
 
bool setFlagSigmaForR (const bool flagSigmaForR_i)
 
void setRequireCKM (bool requireCKM)
 A set method to change the value of requireCKM. More...
 
void setSMSuccess (bool success) const
 A set method to change the success status of the Standard Model update and matching. More...
 
void setYd (const gslpp::matrix< gslpp::complex > &Yd)
 A set method to set the Yukawa matrix of the down-type quarks, \(Y_d\). More...
 
void setYe (const gslpp::matrix< gslpp::complex > &Ye)
 A set method to set the Yukawa matrix of the charged leptons, \(Y_e\). More...
 
void setYu (const gslpp::matrix< gslpp::complex > &Yu)
 A set method to set the Yukawa matrix of the up-type quarks, \(Y_u\). More...
 
virtual const double SigmaeeHee (const double sqrt_s, const double Pe, const double Pp) const
 The \(\sigma(e^+ e^- \to e^+ e^- H)\) in the Standard Model. More...
 
virtual const double SigmaeeHvv (const double sqrt_s, const double Pe, const double Pp) const
 The \(\sigma(e^+ e^- \to \nu \bar{\nu} H)\) in the Standard Model. More...
 
virtual const double SigmaeeZH (const double sqrt_s, const double Pe, const double Pp) const
 The \(\sigma(e^+ e^- \to Z H)\) in the Standard Model. More...
 
 StandardModel ()
 The default constructor. More...
 
const double sW2 () const
 
virtual const double sW2 (const double Mw_i) const
 The square of the sine of the weak mixing angle in the on-shell scheme, denoted as \(s_W^2\). More...
 
const double sW2_MSbar_Approx () const
 The (approximated formula for the) square of the sine of the weak mixing angle in the MSbar scheme, denoted as \(\hat{s}_{W}^2\). See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) More...
 
const double sW2_ND () const
 The square of the sine of the weak mixing angle in the MSbar-ND scheme (w/o decoupling $\alpha\ln(m_t/M_Z)$ terms), denoted as \(\hat{s}_{ND}^2\). See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) (eq. 10.13a/10.13b) More...
 
virtual const double ThetaLnuN () const
 The effective neutrino nucleon LH parameter: ThetaLnuN. More...
 
virtual const double ThetaRnuN () const
 The effective neutrino nucleon RH parameter: ThetaRnuN. More...
 
const double tovers2 (const double cosmin, const double cosmax) const
 
const double uovers2 (const double cosmin, const double cosmax) const
 
const double v () const
 The Higgs vacuum expectation value. More...
 
virtual ~StandardModel ()
 The default destructor. More...
 
- Public Member Functions inherited from QCD
const double AboveTh (const double mu) const
 The active flavour threshold above the scale \(\mu\) as defined in QCD::Thresholds(). More...
 
void addParameters (std::vector< std::string > params_i)
 A method to add parameters that are specific to only one set of observables. More...
 
const double Als (const double mu, const int Nf_in, const orders order=FULLNLO) const
 Computes the running strong coupling \(\alpha_s(\mu)\) with \(N_f\) active flavours in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...
 
const double Als (const double mu, const orders order=FULLNLO, const bool Nf_thr=true) const
 
const double Als4 (const double mu) const
 The value of \(\alpha_s^{\mathrm{FULLNLO}}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\). More...
 
const double AlsByOrder (const double mu, const int Nf_in, const orders order=FULLNLO) const
 
const double AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const
 
const double AlsOLD (const double mu, const orders order=FULLNLO) const
 Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More...
 
const double AlsWithInit (const double mu, const double alsi, const double mu_i, const int nf, const orders order) const
 Computes the running strong coupling \(\alpha_s(\mu)\) from \(\alpha_s(\mu_i)\) in the \(\overline{\mathrm{MS}}\) scheme, where it is forbidden to across a flavour threshold in the RG running from \(\mu_i\) to \(\mu\). More...
 
const double AlsWithLambda (const double mu, const orders order) const
 Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme with the use of \(\Lambda_{\rm QCD}\). More...
 
const double BelowTh (const double mu) const
 The active flavour threshold below the scale \(\mu\) as defined in QCD::Thresholds(). More...
 
const double Beta0 (const double nf) const
 The \(\beta_0(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
const double Beta1 (const double nf) const
 The \(\beta_1(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
const double Beta2 (const double nf) const
 The \(\beta_2(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
const double Beta3 (const double nf) const
 The \(\beta_3(n_f)\) coefficient for a certain number of flavours \(n_f\). More...
 
void CacheShift (double cache[][5], int n) const
 A member used to manage the caching for this class. More...
 
void CacheShift (int cache[][5], int n) const
 
const orders FullOrder (orders order) const
 Return the FULLORDER enum corresponding to order. More...
 
const double Gamma0 (const double nf) const
 The \(\gamma_0\) coefficient used to compute the running of a mass. More...
 
const double Gamma1 (const double nf) const
 The \(\gamma_1\) coefficient used to compute the running of a mass. More...
 
const double Gamma2 (const double nf) const
 The \(\gamma_2\) coefficient used to compute the running of a mass. More...
 
const double getAlsM () const
 A get method to access the value of \(\alpha_s(M_{\alpha_s})\). More...
 
const BParametergetBBd () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More...
 
const BParametergetBBd_subleading () const
 For getting the subleading bag parameters \(R_2 - R_3\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More...
 
const BParametergetBBs () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More...
 
const BParametergetBBs_subleading () const
 For getting the subleading bag parameters \(R_2 - R_3\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More...
 
const BParametergetBD () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta c = 2\) process in the \(D^0\) meson system. More...
 
const BParametergetBK () const
 For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta s = 2\) process in the \(K^0\) meson system. More...
 
const BParametergetBKd1 () const
 
const BParametergetBKd3 () const
 
const double getCF () const
 A get method to access the Casimir factor of QCD. More...
 
const double getMAls () const
 A get method to access the mass scale \(M_{\alpha_s}\) at which the strong coupling constant measurement is provided. More...
 
const MesongetMesons (const QCD::meson m) const
 A get method to access a meson as an object of the type Meson. More...
 
const double getMtpole () const
 A get method to access the pole mass of the top quark. More...
 
const double getMub () const
 A get method to access the threshold between five- and four-flavour theory in GeV. More...
 
const double getMuc () const
 A get method to access the threshold between four- and three-flavour theory in GeV. More...
 
const double getMut () const
 A get method to access the threshold between six- and five-flavour theory in GeV. More...
 
const double getNc () const
 A get method to access the number of colours \(N_c\). More...
 
const double getOptionalParameter (std::string name) const
 A method to get parameters that are specific to only one set of observables. More...
 
const ParticlegetQuarks (const QCD::quark q) const
 A get method to access a quark as an object of the type Particle. More...
 
std::vector< std::string > getUnknownParameters ()
 A method to get the vector of the parameters that have been specified in the configuration file but not being used. More...
 
void initializeBParameter (std::string name_i) const
 A method to initialize B Parameter and the corresponding meson. More...
 
void initializeMeson (QCD::meson meson_i) const
 A method to initialize a meson. More...
 
bool isQCDsuccess () const
 A getter for the QCDsuccess flag. More...
 
const double logLambda (const double nf, orders order) const
 Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More...
 
const double Mbar2Mp (const double mbar, const quark q, const orders order=FULLNNLO) const
 Converts the \(\overline{\mathrm{MS}}\) mass \(m(m)\) to the pole mass. More...
 
const double Mofmu2Mbar (const double m, const double mu, const quark q) const
 Converts a quark running mass at an arbitrary scale to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More...
 
const double Mp2Mbar (const double mp, const quark q, orders order=FULLNNLO) const
 Converts a quark pole mass to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More...
 
const double Mrun (const double mu, const double m, const quark q, const orders order=FULLNNLO) const
 Computes a running quark mass \(m(\mu)\) from \(m(m)\). More...
 
const double Mrun (const double mu_f, const double mu_i, const double m, const quark q, const orders order=FULLNNLO) const
 Runs a quark mass from \(\mu_i\) to \(\mu_f\). More...
 
const double Mrun4 (const double mu_f, const double mu_i, const double m) const
 The running of a mass with the number of flavours \(n_f = 4\). More...
 
const double MS2DRqmass (const double MSbar) const
 Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More...
 
const double MS2DRqmass (const double MSscale, const double MSbar) const
 Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More...
 
const double Nf (const double mu) const
 The number of active flavour at scale \(\mu\). More...
 
const double NfThresholdCorrections (double mu, double M, double als, int nf, orders order) const
 Threshold corrections in matching \(\alpha_s(n_f+1)\) with \(\alpha_s(n_f)\) from eq. (34) of hep-ph/0512060. More...
 
const std::string orderToString (const orders order) const
 Converts an object of the enum type "orders" to the corresponding string. More...
 
 QCD ()
 Constructor. More...
 
void setComputemt (bool computemt)
 A set method to change the value of computemt. More...
 
void setMtpole (double mtpole_in)
 A method to set the pole mass of the top quark. More...
 
void setNc (double Nc)
 A set method to change the number of colours \(N_c\). More...
 
void setOptionalParameter (std::string name, double value)
 A method to set the parameter value for the parameters that are specific to only one set of observables. More...
 
void setQuarkMass (const quark q, const double mass)
 A set method to change the mass of a quark. More...
 
const double Thresholds (const int i) const
 For accessing the active flavour threshold scales. More...
 
- Public Member Functions inherited from Model
void addMissingModelParameter (const std::string &missingParameterName)
 
std::vector< std::string > getmissingModelParameters ()
 
unsigned int getMissingModelParametersCount ()
 
std::string getModelName () const
 A method to fetch the name of the model. More...
 
const double & getModelParam (std::string name) const
 
bool isModelFWC_DF2 () const
 
bool isModelGeneralTHDM () const
 
bool isModelGeorgiMachacek () const
 
bool IsModelInitialized () const
 A method to check if the model is initialized. More...
 
bool isModelLinearized () const
 
bool isModelNPquadratic () const
 
bool isModelParam (std::string name) const
 
bool isModelSUSY () const
 
bool isModelTHDM () const
 
bool isModelTHDMW () const
 
bool IsUpdateError () const
 A method to check if there was any error in the model update process. More...
 
 Model ()
 The default constructor. More...
 
void raiseMissingModelParameterCount ()
 
void setModelFWC_DF2 ()
 
void setModelGeneralTHDM ()
 
void setModelGeorgiMachacek ()
 
void setModelInitialized (bool ModelInitialized)
 A set method to fix the failure or success of the initialization of the model. More...
 
void setModelLinearized (bool linearized=true)
 
void setModelName (const std::string name)
 A method to set the name of the model. More...
 
void setModelNPquadratic (bool NPquadratic=true)
 
void setModelSUSY ()
 
void setModelTHDM ()
 
void setModelTHDMW ()
 
void setSliced (bool Sliced)
 
void setUpdateError (bool UpdateError)
 A set method to fix the update status as success or failure. More...
 
virtual ~Model ()
 The default destructor. More...
 

Static Public Attributes

static const int NNPSMEFTd6MFVVars = 128+1
 
static std::string NPSMEFTd6MFVVars [NNPSMEFTd6MFVVars]
 
- Static Public Attributes inherited from NPSMEFTd6General
static const int NNPSMEFTd6GeneralVars = 2708-208 + 79
 The number of the model parameters in NPSMEFTd6General (including the 18 parameters needed for the SM and 79 auxiliary parameters). More...
 
static const std::string NPSMEFTd6GeneralVars [NNPSMEFTd6GeneralVars]
 A string array containing the labels of the model parameters in NPSMEFTd6General. More...
 
- Static Public Attributes inherited from StandardModel
static const double GeVminus2_to_nb = 389379.338
 
static const double Mw_error = 0.00001
 The target accuracy of the iterative calculation of the \(W\)-boson mass in units of GeV. More...
 
static const int NSMvars = 28
 The number of the model parameters in StandardModel. More...
 
static const int NumSMParamsForEWPO = 35
 The number of the SM parameters that are relevant to the EW precision observables. More...
 
static std::string SMvars [NSMvars]
 A string array containing the labels of the model parameters in StandardModel. More...
 
- Static Public Attributes inherited from QCD
static const int NQCDvars = 11
 The number of model parameters in QCD. More...
 
static std::string QCDvars [NQCDvars]
 An array containing the labels under which all QCD parameters are stored in a vector of ModelParameter via InputParser::ReadParameters(). More...
 

Protected Member Functions

void setNPSMEFTd6GeneralParameters ()
 An auxiliary method to set the WC of the general class. More...
 
virtual void setParameter (const std::string name, const double &value)
 
- Protected Member Functions inherited from NPSMEFTd6General
gslpp::complex CfB_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f. More...
 
gslpp::complex CfG_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f. More...
 
gslpp::complex CfH_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f. More...
 
gslpp::complex CfH_diag_mu (const Particle f, const double mu) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f. More...
 
gslpp::complex CfW_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f. More...
 
void ChangeToEvolutorsBasisPureSM ()
 This function computes the SM parameters needed for the evolutor, neglecting any NP contribution. More...
 
void ChangeToEvolutorsBasisSMEFTtoSM ()
 This function computes the SM parameters needed for the evolutor, including a LO approximation to NP contributions where the Wilson coefficients are evaluated at the UV. More...
 
double CHF1_diag (const Particle F) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F. More...
 
double CHF3_diag (const Particle F) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F. More...
 
gslpp::complex CHF3CC_diag (const Particle F) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to charged-current modification, e.g. quarks u d (family diagonal). More...
 
double CHf_diag (const Particle f) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f. More...
 
gslpp::complex CHud_diag (const Particle u) const
 The diagonal entry of the dimension-6 operator coefficient \(C_{Hud}\) corresponding to particle f. More...
 
void computeQuarkMassesAndCKMFromYukawas ()
 The method to compute the Yukawas matrix. More...
 
void setSMEFTEvolWC (RGESolver &RGevol)
 An auxiliary method to set the WC on the evolutor. More...
 
- Protected Member Functions inherited from StandardModel
const double AFB_NoISR_l (const QCD::lepton l_flavor, const double s) const
 
const double AFB_NoISR_q (const QCD::quark q_flavor, const double s) const
 
bool checkEWPOscheme (const std::string scheme) const
 A method to check if a given scheme name in string form is valid. More...
 
virtual void computeCKM ()
 The method to compute the CKM matrix. More...
 
virtual void computeYukawas ()
 The method to compute the Yukawas matrix. More...
 
double Delta_EWQCD (const QCD::quark q) const
 The non-factorizable EW-QCD corrections to the partial widths for \(Z\to q\bar{q}\), denoted as \(\Delta_{\mathrm{EW/QCD}}\). More...
 
const double getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_charm133 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_charm167 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_charm172 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_charm183 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_charm189 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_charm192 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_charm196 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_charm200 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_charm202 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_charm205 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_charm207 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_mu130 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_mu136 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_mu161 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_mu172 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_mu183 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_mu189 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_mu192 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_mu196 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_mu200 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_mu202 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_mu205 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_mu207 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_tau130 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_tau136 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_tau161 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_tau172 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_tau183 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_tau189 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_tau192 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_tau196 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_tau200 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_tau202 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_tau205 (double x) const
 
const double getIntegrand_AFBnumeratorWithISR_tau207 (double x) const
 
const double getIntegrand_dsigmaBox_bottom130 (double x) const
 
const double getIntegrand_dsigmaBox_bottom133 (double x) const
 
const double getIntegrand_dsigmaBox_bottom136 (double x) const
 
const double getIntegrand_dsigmaBox_bottom161 (double x) const
 
const double getIntegrand_dsigmaBox_bottom167 (double x) const
 
const double getIntegrand_dsigmaBox_bottom172 (double x) const
 
const double getIntegrand_dsigmaBox_bottom183 (double x) const
 
const double getIntegrand_dsigmaBox_bottom189 (double x) const
 
const double getIntegrand_dsigmaBox_bottom192 (double x) const
 
const double getIntegrand_dsigmaBox_bottom196 (double x) const
 
const double getIntegrand_dsigmaBox_bottom200 (double x) const
 
const double getIntegrand_dsigmaBox_bottom202 (double x) const
 
const double getIntegrand_dsigmaBox_bottom205 (double x) const
 
const double getIntegrand_dsigmaBox_bottom207 (double x) const
 
const double getIntegrand_dsigmaBox_charm130 (double x) const
 
const double getIntegrand_dsigmaBox_charm133 (double x) const
 
const double getIntegrand_dsigmaBox_charm136 (double x) const
 
const double getIntegrand_dsigmaBox_charm161 (double x) const
 
const double getIntegrand_dsigmaBox_charm167 (double x) const
 
const double getIntegrand_dsigmaBox_charm172 (double x) const
 
const double getIntegrand_dsigmaBox_charm183 (double x) const
 
const double getIntegrand_dsigmaBox_charm189 (double x) const
 
const double getIntegrand_dsigmaBox_charm192 (double x) const
 
const double getIntegrand_dsigmaBox_charm196 (double x) const
 
const double getIntegrand_dsigmaBox_charm200 (double x) const
 
const double getIntegrand_dsigmaBox_charm202 (double x) const
 
const double getIntegrand_dsigmaBox_charm205 (double x) const
 
const double getIntegrand_dsigmaBox_charm207 (double x) const
 
const double getIntegrand_dsigmaBox_down130 (double x) const
 
const double getIntegrand_dsigmaBox_down133 (double x) const
 
const double getIntegrand_dsigmaBox_down136 (double x) const
 
const double getIntegrand_dsigmaBox_down161 (double x) const
 
const double getIntegrand_dsigmaBox_down167 (double x) const
 
const double getIntegrand_dsigmaBox_down172 (double x) const
 
const double getIntegrand_dsigmaBox_down183 (double x) const
 
const double getIntegrand_dsigmaBox_down189 (double x) const
 
const double getIntegrand_dsigmaBox_down192 (double x) const
 
const double getIntegrand_dsigmaBox_down196 (double x) const
 
const double getIntegrand_dsigmaBox_down200 (double x) const
 
const double getIntegrand_dsigmaBox_down202 (double x) const
 
const double getIntegrand_dsigmaBox_down205 (double x) const
 
const double getIntegrand_dsigmaBox_down207 (double x) const
 
const double getIntegrand_dsigmaBox_mu130 (double x) const
 
const double getIntegrand_dsigmaBox_mu133 (double x) const
 
const double getIntegrand_dsigmaBox_mu136 (double x) const
 
const double getIntegrand_dsigmaBox_mu161 (double x) const
 
const double getIntegrand_dsigmaBox_mu167 (double x) const
 
const double getIntegrand_dsigmaBox_mu172 (double x) const
 
const double getIntegrand_dsigmaBox_mu183 (double x) const
 
const double getIntegrand_dsigmaBox_mu189 (double x) const
 
const double getIntegrand_dsigmaBox_mu192 (double x) const
 
const double getIntegrand_dsigmaBox_mu196 (double x) const
 
const double getIntegrand_dsigmaBox_mu200 (double x) const
 
const double getIntegrand_dsigmaBox_mu202 (double x) const
 
const double getIntegrand_dsigmaBox_mu205 (double x) const
 
const double getIntegrand_dsigmaBox_mu207 (double x) const
 
const double getIntegrand_dsigmaBox_strange130 (double x) const
 
const double getIntegrand_dsigmaBox_strange133 (double x) const
 
const double getIntegrand_dsigmaBox_strange136 (double x) const
 
const double getIntegrand_dsigmaBox_strange161 (double x) const
 
const double getIntegrand_dsigmaBox_strange167 (double x) const
 
const double getIntegrand_dsigmaBox_strange172 (double x) const
 
const double getIntegrand_dsigmaBox_strange183 (double x) const
 
const double getIntegrand_dsigmaBox_strange189 (double x) const
 
const double getIntegrand_dsigmaBox_strange192 (double x) const
 
const double getIntegrand_dsigmaBox_strange196 (double x) const
 
const double getIntegrand_dsigmaBox_strange200 (double x) const
 
const double getIntegrand_dsigmaBox_strange202 (double x) const
 
const double getIntegrand_dsigmaBox_strange205 (double x) const
 
const double getIntegrand_dsigmaBox_strange207 (double x) const
 
const double getIntegrand_dsigmaBox_tau130 (double x) const
 
const double getIntegrand_dsigmaBox_tau133 (double x) const
 
const double getIntegrand_dsigmaBox_tau136 (double x) const
 
const double getIntegrand_dsigmaBox_tau161 (double x) const
 
const double getIntegrand_dsigmaBox_tau167 (double x) const
 
const double getIntegrand_dsigmaBox_tau172 (double x) const
 
const double getIntegrand_dsigmaBox_tau183 (double x) const
 
const double getIntegrand_dsigmaBox_tau189 (double x) const
 
const double getIntegrand_dsigmaBox_tau192 (double x) const
 
const double getIntegrand_dsigmaBox_tau196 (double x) const
 
const double getIntegrand_dsigmaBox_tau200 (double x) const
 
const double getIntegrand_dsigmaBox_tau202 (double x) const
 
const double getIntegrand_dsigmaBox_tau205 (double x) const
 
const double getIntegrand_dsigmaBox_tau207 (double x) const
 
const double getIntegrand_dsigmaBox_up130 (double x) const
 
const double getIntegrand_dsigmaBox_up133 (double x) const
 
const double getIntegrand_dsigmaBox_up136 (double x) const
 
const double getIntegrand_dsigmaBox_up161 (double x) const
 
const double getIntegrand_dsigmaBox_up167 (double x) const
 
const double getIntegrand_dsigmaBox_up172 (double x) const
 
const double getIntegrand_dsigmaBox_up183 (double x) const
 
const double getIntegrand_dsigmaBox_up189 (double x) const
 
const double getIntegrand_dsigmaBox_up192 (double x) const
 
const double getIntegrand_dsigmaBox_up196 (double x) const
 
const double getIntegrand_dsigmaBox_up200 (double x) const
 
const double getIntegrand_dsigmaBox_up202 (double x) const
 
const double getIntegrand_dsigmaBox_up205 (double x) const
 
const double getIntegrand_dsigmaBox_up207 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom130 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom133 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom136 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom161 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom167 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom172 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom183 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom189 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom192 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom196 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom200 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom202 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom205 (double x) const
 
const double getIntegrand_sigmaWithISR_bottom207 (double x) const
 
const double getIntegrand_sigmaWithISR_charm130 (double x) const
 
const double getIntegrand_sigmaWithISR_charm133 (double x) const
 
const double getIntegrand_sigmaWithISR_charm136 (double x) const
 
const double getIntegrand_sigmaWithISR_charm161 (double x) const
 
const double getIntegrand_sigmaWithISR_charm167 (double x) const
 
const double getIntegrand_sigmaWithISR_charm172 (double x) const
 
const double getIntegrand_sigmaWithISR_charm183 (double x) const
 
const double getIntegrand_sigmaWithISR_charm189 (double x) const
 
const double getIntegrand_sigmaWithISR_charm192 (double x) const
 
const double getIntegrand_sigmaWithISR_charm196 (double x) const
 
const double getIntegrand_sigmaWithISR_charm200 (double x) const
 
const double getIntegrand_sigmaWithISR_charm202 (double x) const
 
const double getIntegrand_sigmaWithISR_charm205 (double x) const
 
const double getIntegrand_sigmaWithISR_charm207 (double x) const
 
const double getIntegrand_sigmaWithISR_down130 (double x) const
 
const double getIntegrand_sigmaWithISR_down133 (double x) const
 
const double getIntegrand_sigmaWithISR_down136 (double x) const
 
const double getIntegrand_sigmaWithISR_down161 (double x) const
 
const double getIntegrand_sigmaWithISR_down167 (double x) const
 
const double getIntegrand_sigmaWithISR_down172 (double x) const
 
const double getIntegrand_sigmaWithISR_down183 (double x) const
 
const double getIntegrand_sigmaWithISR_down189 (double x) const
 
const double getIntegrand_sigmaWithISR_down192 (double x) const
 
const double getIntegrand_sigmaWithISR_down196 (double x) const
 
const double getIntegrand_sigmaWithISR_down200 (double x) const
 
const double getIntegrand_sigmaWithISR_down202 (double x) const
 
const double getIntegrand_sigmaWithISR_down205 (double x) const
 
const double getIntegrand_sigmaWithISR_down207 (double x) const
 
const double getIntegrand_sigmaWithISR_mu130 (double x) const
 
const double getIntegrand_sigmaWithISR_mu136 (double x) const
 
const double getIntegrand_sigmaWithISR_mu161 (double x) const
 
const double getIntegrand_sigmaWithISR_mu172 (double x) const
 
const double getIntegrand_sigmaWithISR_mu183 (double x) const
 
const double getIntegrand_sigmaWithISR_mu189 (double x) const
 
const double getIntegrand_sigmaWithISR_mu192 (double x) const
 
const double getIntegrand_sigmaWithISR_mu196 (double x) const
 
const double getIntegrand_sigmaWithISR_mu200 (double x) const
 
const double getIntegrand_sigmaWithISR_mu202 (double x) const
 
const double getIntegrand_sigmaWithISR_mu205 (double x) const
 
const double getIntegrand_sigmaWithISR_mu207 (double x) const
 
const double getIntegrand_sigmaWithISR_strange130 (double x) const
 
const double getIntegrand_sigmaWithISR_strange133 (double x) const
 
const double getIntegrand_sigmaWithISR_strange136 (double x) const
 
const double getIntegrand_sigmaWithISR_strange161 (double x) const
 
const double getIntegrand_sigmaWithISR_strange167 (double x) const
 
const double getIntegrand_sigmaWithISR_strange172 (double x) const
 
const double getIntegrand_sigmaWithISR_strange183 (double x) const
 
const double getIntegrand_sigmaWithISR_strange189 (double x) const
 
const double getIntegrand_sigmaWithISR_strange192 (double x) const
 
const double getIntegrand_sigmaWithISR_strange196 (double x) const
 
const double getIntegrand_sigmaWithISR_strange200 (double x) const
 
const double getIntegrand_sigmaWithISR_strange202 (double x) const
 
const double getIntegrand_sigmaWithISR_strange205 (double x) const
 
const double getIntegrand_sigmaWithISR_strange207 (double x) const
 
const double getIntegrand_sigmaWithISR_tau130 (double x) const
 
const double getIntegrand_sigmaWithISR_tau136 (double x) const
 
const double getIntegrand_sigmaWithISR_tau161 (double x) const
 
const double getIntegrand_sigmaWithISR_tau172 (double x) const
 
const double getIntegrand_sigmaWithISR_tau183 (double x) const
 
const double getIntegrand_sigmaWithISR_tau189 (double x) const
 
const double getIntegrand_sigmaWithISR_tau192 (double x) const
 
const double getIntegrand_sigmaWithISR_tau196 (double x) const
 
const double getIntegrand_sigmaWithISR_tau200 (double x) const
 
const double getIntegrand_sigmaWithISR_tau202 (double x) const
 
const double getIntegrand_sigmaWithISR_tau205 (double x) const
 
const double getIntegrand_sigmaWithISR_tau207 (double x) const
 
const double getIntegrand_sigmaWithISR_up130 (double x) const
 
const double getIntegrand_sigmaWithISR_up133 (double x) const
 
const double getIntegrand_sigmaWithISR_up136 (double x) const
 
const double getIntegrand_sigmaWithISR_up161 (double x) const
 
const double getIntegrand_sigmaWithISR_up167 (double x) const
 
const double getIntegrand_sigmaWithISR_up172 (double x) const
 
const double getIntegrand_sigmaWithISR_up183 (double x) const
 
const double getIntegrand_sigmaWithISR_up189 (double x) const
 
const double getIntegrand_sigmaWithISR_up192 (double x) const
 
const double getIntegrand_sigmaWithISR_up196 (double x) const
 
const double getIntegrand_sigmaWithISR_up200 (double x) const
 
const double getIntegrand_sigmaWithISR_up202 (double x) const
 
const double getIntegrand_sigmaWithISR_up205 (double x) const
 
const double getIntegrand_sigmaWithISR_up207 (double x) const
 
const double Integrand_AFBnumeratorWithISR_l (double x, const QCD::lepton l_flavor, const double s) const
 
const double Integrand_AFBnumeratorWithISR_q (double x, const QCD::quark q_flavor, const double s) const
 
const double Integrand_dsigmaBox_l (double cosTheta, const QCD::lepton l_flavor, const double s) const
 
const double Integrand_dsigmaBox_q (double cosTheta, const QCD::quark q_flavor, const double s) const
 
const double Integrand_sigmaWithISR_l (double x, const QCD::lepton l_flavor, const double s) const
 
const double Integrand_sigmaWithISR_q (double x, const QCD::quark q_flavor, const double s) const
 
double m_q (const QCD::quark q, const double mu, const orders order=FULLNLO) const
 
double RAq (const QCD::quark q) const
 The radiator factor associated with the final-state QED and QCD corrections to the the axial-vector-current interactions, \(R_A^q(M_Z^2)\). More...
 
double resumKappaZ (const double DeltaRho[orders_EW_size], const double deltaKappa_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
 A method to compute the real part of the effetvive coupling \(\kappa_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More...
 
double resumMw (const double Mw_i, const double DeltaRho[orders_EW_size], const double DeltaR_rem[orders_EW_size]) const
 A method to compute the \(W\)-boson mass from \(\Delta\rho\) and \(\Delta r_{\mathrm{rem}}\). More...
 
double resumRhoZ (const double DeltaRho[orders_EW_size], const double deltaRho_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const
 A method to compute the real part of the effective coupling \(\rho_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More...
 
double RVh () const
 The singlet vector corrections to the hadronic \(Z\)-boson width, denoted as \(R_V^h\). More...
 
double RVq (const QCD::quark q) const
 The radiator factor associated with the final-state QED and QCD corrections to the the vector-current interactions, \(R_V^q(M_Z^2)\). More...
 
double SchemeToDouble (const std::string scheme) const
 A method to convert a given scheme name in string form into a floating-point number with double precision. More...
 
const double sigma_NoISR_l (const QCD::lepton l_flavor, const double s) const
 
const double sigma_NoISR_q (const QCD::quark q_flavor, const double s) const
 
double taub () const
 Top-mass corrections to the \(Zb\bar{b}\) vertex, denoted by \(\tau_b\). More...
 
- Protected Member Functions inherited from QCD
const double MassOfNf (int nf) const
 The Mbar mass of the heaviest quark in the theory with Nf active flavour. More...
 

Protected Attributes

double CdB_0_LNP = 0.
 
double CdB_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{Hq}^{(1)})_{ij}\). More...
 
double CdB_u_LNP = 0.
 
double Cdd_00_LNP = 0.
 
double Cdd_0d_LNP = 0.
 
double Cdd_d0_LNP = 0.
 
double Cdd_dd_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ud}^{(1)})_{ijkm}\). More...
 
double CdG_0_LNP = 0.
 
double CdG_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{dW})_{ij}\). More...
 
double CdG_u_LNP = 0.
 
double CdH_0_LNP = 0.
 
double CdH_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{dG})_{ij}\). More...
 
double CdH_u_LNP = 0.
 
double CdW_0_LNP = 0.
 
double CdW_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{dB})_{ij}\). More...
 
double CdW_u_LNP = 0.
 
double Ced_0_LNP = 0.
 
double Ced_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qq}^{(1)})_{ijkm}\). More...
 
double Cee_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{le})_{ijkm}\). More...
 
double Ceu_0_LNP = 0.
 
double Ceu_u_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ld})_{ijkm}\). More...
 
double CHd_0_LNP = 0.
 
double CHd_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{Hud})_{ij}\). More...
 
double CHe_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ll})_{ijkm}\). More...
 
double CHl1_LNP = 0.
 < Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{Hl}^{(1)})_{ij}\). More...
 
double CHl3_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{He})_{ij}\). More...
 
double CHq1_0_LNP = 0.
 
double CHq1_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{Hq}^{(3)})_{ij}\). More...
 
double CHq1_u_LNP = 0.
 
double CHq3_0_LNP = 0.
 
double CHq3_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{Hu})_{ij}\). More...
 
double CHq3_u_LNP = 0.
 
double CHu_0_LNP = 0.
 
double CHu_u_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{Hd})_{ij}\). More...
 
double CHud_ud_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{lq}^{(1)})_{ijkm}\). More...
 
double Cld_0_LNP = 0.
 
double Cld_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ed})_{ijkm}\). More...
 
double Cle_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{uH})_{ij}\). More...
 
double Cll_aabb_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ll})_{ijkm}\). More...
 
double Cll_abba_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ee})_{ijkm}\). More...
 
double Clq1_0_LNP = 0.
 
double Clq1_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{lq}^{(3)})_{ijkm}\). More...
 
double Clq1_u_LNP = 0.
 
double Clq3_0_LNP = 0.
 
double Clq3_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qe})_{ijkm}\). More...
 
double Clq3_u_LNP = 0.
 
double Clu_0_LNP = 0.
 
double Clu_u_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{eu})_{ijkm}\). More...
 
double Cqd1_00_LNP = 0.
 
double Cqd1_0d_LNP = 0.
 
double Cqd1_d0_LNP = 0.
 
double Cqd1_dd_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qd}^{(8)})_{ijkm}\). More...
 
double Cqd1_u0_LNP = 0.
 
double Cqd1_ud_LNP = 0.
 
double Cqd8_00_LNP = 0.
 
double Cqd8_0d_LNP = 0.
 
double Cqd8_d0_LNP = 0.
 
double Cqd8_dd_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{quqd}^{(1)})_{ijkm}\). More...
 
double Cqd8_u0_LNP = 0.
 
double Cqd8_ud_LNP = 0.
 
double Cqe_0_LNP = 0.
 
double Cqe_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{lu})_{ijkm}\). More...
 
double Cqe_u_LNP = 0.
 
double Cqq1_00_LNP = 0.
 
double Cqq1_0d_LNP = 0.
 
double Cqq1_0u_LNP = 0.
 
double Cqq1_d0_LNP = 0.
 
double Cqq1_dd_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qq}^{(3)})_{ijkm}\). More...
 
double Cqq1_du_LNP = 0.
 
double Cqq1_u0_LNP = 0.
 
double Cqq1_ud_LNP = 0.
 
double Cqq1_uu_LNP = 0.
 
double Cqq3_00_LNP = 0.
 
double Cqq3_0d_LNP = 0.
 
double Cqq3_0u_LNP = 0.
 
double Cqq3_d0_LNP = 0.
 
double Cqq3_dd_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{uu})_{ijkm}\). More...
 
double Cqq3_du_LNP = 0.
 
double Cqq3_u0_LNP = 0.
 
double Cqq3_ud_LNP = 0.
 
double Cqq3_uu_LNP = 0.
 
double Cqu1_00_LNP = 0.
 
double Cqu1_0u_LNP = 0.
 
double Cqu1_d0_LNP = 0.
 
double Cqu1_du_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qu}^{(8)})_{ijkm}\). More...
 
double Cqu1_u0_LNP = 0.
 
double Cqu1_uu_LNP = 0.
 
double Cqu8_00_LNP = 0.
 
double Cqu8_0u_LNP = 0.
 
double Cqu8_d0_LNP = 0.
 
double Cqu8_du_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qd}^{(1)})_{ijkm}\). More...
 
double Cqu8_u0_LNP = 0.
 
double Cqu8_uu_LNP = 0.
 
double Cquqd1_00_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{quqd}^{(8)})_{ijkm}\). More...
 
double Cquqd8_00_LNP = 0.
 
double CuB_0_LNP = 0.
 
double CuB_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{dH})_{ij}\). More...
 
double CuB_u_LNP = 0.
 
double Cud1_00_LNP = 0.
 
double Cud1_0d_LNP = 0.
 
double Cud1_u0_LNP = 0.
 
double Cud1_ud_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ud}^{(8)})_{ijkm}\). More...
 
double Cud8_00_LNP = 0.
 
double Cud8_0d_LNP = 0.
 
double Cud8_u0_LNP = 0.
 
double Cud8_ud_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qu}^{(1)})_{ijkm}\). More...
 
double CuG_0_LNP = 0.
 
double CuG_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{uW})_{ij}\). More...
 
double CuG_u_LNP = 0.
 
double CuH_0_LNP = 0.
 
double CuH_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{uG})_{ij}\). More...
 
double CuH_u_LNP = 0.
 
double Cuu_00_LNP = 0.
 
double Cuu_0u_LNP = 0.
 
double Cuu_u0_LNP = 0.
 
double Cuu_uu_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{dd})_{ijkm}\). More...
 
double CuW_0_LNP = 0.
 
double CuW_d_LNP = 0.
 Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{uB})_{ij}\). More...
 
double CuW_u_LNP = 0.
 
- Protected Attributes inherited from NPSMEFTd6General
double ai2G
 
double ai3G
 
double aiA
 
double aiB
 
double aiG
 
double aiH
 
double aiHB
 
double aiHd
 
double aiHe
 
double aiHL
 
double aiHQ
 
double aiHu
 
double aiHW
 
double aipHL
 
double aipHQ
 
double aiT
 
double aiu
 
double aiuG
 
double aiWW
 
double aleMz
 The em constant at Mz. More...
 
double BrHexo = 0.
 The branching ratio of exotic (not invisible) Higgs decays. More...
 
double BrHinv = 0.
 The branching ratio of invisible Higgs decays. More...
 
double C1Htotal
 The C1 coefficient controlling the H^3 corrections to the total Higgs width from the Higgs trilinear coupling. More...
 
double cAsch
 
double CdB_11i_LNP = 0.
 
double CdB_11r_LNP = 0.
 
double CdB_12i_LNP = 0.
 
double CdB_12r_LNP = 0.
 
double CdB_13i_LNP = 0.
 
double CdB_13r_LNP = 0.
 
double CdB_21i_LNP = 0.
 
double CdB_21r_LNP = 0.
 
double CdB_22i_LNP = 0.
 
double CdB_22r_LNP = 0.
 
double CdB_23i_LNP = 0.
 
double CdB_23r_LNP = 0.
 
double CdB_31i_LNP = 0.
 
double CdB_31r_LNP = 0.
 
double CdB_32i_LNP = 0.
 
double CdB_32r_LNP = 0.
 
double CdB_33i_LNP = 0.
 The dimension-6 operator coefficient \((C_{dB})_{ij}\) (Imaginary part). More...
 
double CdB_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{dB})_{ij}\) (Real part and pure real operator). More...
 
double CDB_LNP = 0
 The dimension-6 operator coefficient \(C_{DB}\). More...
 
double Cdd_1111r_LNP = 0.
 
double Cdd_1112i_LNP = 0.
 
double Cdd_1112r_LNP = 0.
 
double Cdd_1113i_LNP = 0.
 
double Cdd_1113r_LNP = 0.
 
double Cdd_1122r_LNP = 0.
 
double Cdd_1123i_LNP = 0.
 
double Cdd_1123r_LNP = 0.
 
double Cdd_1133r_LNP = 0.
 
double Cdd_1212i_LNP = 0.
 
double Cdd_1212r_LNP = 0.
 
double Cdd_1213i_LNP = 0.
 
double Cdd_1213r_LNP = 0.
 
double Cdd_1221r_LNP = 0.
 
double Cdd_1222i_LNP = 0.
 
double Cdd_1222r_LNP = 0.
 
double Cdd_1223i_LNP = 0.
 
double Cdd_1223r_LNP = 0.
 
double Cdd_1231i_LNP = 0.
 
double Cdd_1231r_LNP = 0.
 
double Cdd_1232i_LNP = 0.
 
double Cdd_1232r_LNP = 0.
 
double Cdd_1233i_LNP = 0.
 
double Cdd_1233r_LNP = 0.
 
double Cdd_1313i_LNP = 0.
 
double Cdd_1313r_LNP = 0.
 
double Cdd_1322i_LNP = 0.
 
double Cdd_1322r_LNP = 0.
 
double Cdd_1323i_LNP = 0.
 
double Cdd_1323r_LNP = 0.
 
double Cdd_1331r_LNP = 0.
 
double Cdd_1332i_LNP = 0.
 
double Cdd_1332r_LNP = 0.
 
double Cdd_1333i_LNP = 0.
 
double Cdd_1333r_LNP = 0.
 
double Cdd_2222r_LNP = 0.
 
double Cdd_2223i_LNP = 0.
 
double Cdd_2223r_LNP = 0.
 
double Cdd_2233r_LNP = 0.
 
double Cdd_2323i_LNP = 0.
 
double Cdd_2323r_LNP = 0.
 
double Cdd_2332r_LNP = 0.
 
double Cdd_2333i_LNP = 0.
 The dimension-6 operator coefficient \((C_{dd})_{ijkm}\) (Imaginary part). More...
 
double Cdd_2333r_LNP = 0.
 
double Cdd_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{dd})_{ijkm}\) (Real part and pure real operator). More...
 
double CdG_11i_LNP = 0.
 
double CdG_11r_LNP = 0.
 
double CdG_12i_LNP = 0.
 
double CdG_12r_LNP = 0.
 
double CdG_13i_LNP = 0.
 
double CdG_13r_LNP = 0.
 
double CdG_21i_LNP = 0.
 
double CdG_21r_LNP = 0.
 
double CdG_22i_LNP = 0.
 
double CdG_22r_LNP = 0.
 
double CdG_23i_LNP = 0.
 
double CdG_23r_LNP = 0.
 
double CdG_31i_LNP = 0.
 
double CdG_31r_LNP = 0.
 
double CdG_32i_LNP = 0.
 
double CdG_32r_LNP = 0.
 
double CdG_33i_LNP = 0.
 The dimension-6 operator coefficient \((C_{dG})_{ij}\) (Imaginary part). More...
 
double CdG_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{dG})_{ij}\) (Real part and pure real operator). More...
 
double CdH_11i_LNP = 0.
 
double CdH_11r_LNP = 0.
 
double CdH_12i_LNP = 0.
 
double CdH_12r_LNP = 0.
 
double CdH_13i_LNP = 0.
 
double CdH_13r_LNP = 0.
 
double CdH_21i_LNP = 0.
 
double CdH_21r_LNP = 0.
 
double CdH_22i_LNP = 0.
 
double CdH_22r_LNP = 0.
 
double CdH_23i_LNP = 0.
 
double CdH_23r_LNP = 0.
 
double CdH_31i_LNP = 0.
 
double CdH_31r_LNP = 0.
 
double CdH_32i_LNP = 0.
 
double CdH_32r_LNP = 0.
 
double CdH_33i_LNP = 0.
 The dimension-6 operator coefficient \((C_{dH})_{ij}\) (Imaginary part). More...
 
double CdH_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{dH})_{ij}\) (Real part and pure real operator). More...
 
double CdW_11i_LNP = 0.
 
double CdW_11r_LNP = 0.
 
double CdW_12i_LNP = 0.
 
double CdW_12r_LNP = 0.
 
double CdW_13i_LNP = 0.
 
double CdW_13r_LNP = 0.
 
double CdW_21i_LNP = 0.
 
double CdW_21r_LNP = 0.
 
double CdW_22i_LNP = 0.
 
double CdW_22r_LNP = 0.
 
double CdW_23i_LNP = 0.
 
double CdW_23r_LNP = 0.
 
double CdW_31i_LNP = 0.
 
double CdW_31r_LNP = 0.
 
double CdW_32i_LNP = 0.
 
double CdW_32r_LNP = 0.
 
double CdW_33i_LNP = 0.
 The dimension-6 operator coefficient \((C_{dW})_{ij}\) (Imaginary part). More...
 
double CdW_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{dW})_{ij}\) (Real part and pure real operator). More...
 
double CDW_LNP = 0
 The dimension-6 operator coefficient \(C_{DW}\). More...
 
double CeB_11i_LNP = 0.
 
double CeB_11r_LNP = 0.
 
double CeB_12i_LNP = 0.
 
double CeB_12r_LNP = 0.
 
double CeB_13i_LNP = 0.
 
double CeB_13r_LNP = 0.
 
double CeB_21i_LNP = 0.
 
double CeB_21r_LNP = 0.
 
double CeB_22i_LNP = 0.
 
double CeB_22r_LNP = 0.
 
double CeB_23i_LNP = 0.
 
double CeB_23r_LNP = 0.
 
double CeB_31i_LNP = 0.
 
double CeB_31r_LNP = 0.
 
double CeB_32i_LNP = 0.
 
double CeB_32r_LNP = 0.
 
double CeB_33i_LNP = 0.
 The dimension-6 operator coefficient \((C_{eB})_{ij}\) (Imaginary part). More...
 
double CeB_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{eB})_{ij}\) (Real part and pure real operator). More...
 
double Ced_1111r_LNP = 0.
 
double Ced_1112i_LNP = 0.
 
double Ced_1112r_LNP = 0.
 
double Ced_1113i_LNP = 0.
 
double Ced_1113r_LNP = 0.
 
double Ced_1122r_LNP = 0.
 
double Ced_1123i_LNP = 0.
 
double Ced_1123r_LNP = 0.
 
double Ced_1133r_LNP = 0.
 
double Ced_1211i_LNP = 0.
 
double Ced_1211r_LNP = 0.
 
double Ced_1212i_LNP = 0.
 
double Ced_1212r_LNP = 0.
 
double Ced_1213i_LNP = 0.
 
double Ced_1213r_LNP = 0.
 
double Ced_1221i_LNP = 0.
 
double Ced_1221r_LNP = 0.
 
double Ced_1222i_LNP = 0.
 
double Ced_1222r_LNP = 0.
 
double Ced_1223i_LNP = 0.
 
double Ced_1223r_LNP = 0.
 
double Ced_1231i_LNP = 0.
 
double Ced_1231r_LNP = 0.
 
double Ced_1232i_LNP = 0.
 
double Ced_1232r_LNP = 0.
 
double Ced_1233i_LNP = 0.
 
double Ced_1233r_LNP = 0.
 
double Ced_1311i_LNP = 0.
 
double Ced_1311r_LNP = 0.
 
double Ced_1312i_LNP = 0.
 
double Ced_1312r_LNP = 0.
 
double Ced_1313i_LNP = 0.
 
double Ced_1313r_LNP = 0.
 
double Ced_1321i_LNP = 0.
 
double Ced_1321r_LNP = 0.
 
double Ced_1322i_LNP = 0.
 
double Ced_1322r_LNP = 0.
 
double Ced_1323i_LNP = 0.
 
double Ced_1323r_LNP = 0.
 
double Ced_1331i_LNP = 0.
 
double Ced_1331r_LNP = 0.
 
double Ced_1332i_LNP = 0.
 
double Ced_1332r_LNP = 0.
 
double Ced_1333i_LNP = 0.
 
double Ced_1333r_LNP = 0.
 
double Ced_2211r_LNP = 0.
 
double Ced_2212i_LNP = 0.
 
double Ced_2212r_LNP = 0.
 
double Ced_2213i_LNP = 0.
 
double Ced_2213r_LNP = 0.
 
double Ced_2222r_LNP = 0.
 
double Ced_2223i_LNP = 0.
 
double Ced_2223r_LNP = 0.
 
double Ced_2233r_LNP = 0.
 
double Ced_2311i_LNP = 0.
 
double Ced_2311r_LNP = 0.
 
double Ced_2312i_LNP = 0.
 
double Ced_2312r_LNP = 0.
 
double Ced_2313i_LNP = 0.
 
double Ced_2313r_LNP = 0.
 
double Ced_2321i_LNP = 0.
 
double Ced_2321r_LNP = 0.
 
double Ced_2322i_LNP = 0.
 
double Ced_2322r_LNP = 0.
 
double Ced_2323i_LNP = 0.
 
double Ced_2323r_LNP = 0.
 
double Ced_2331i_LNP = 0.
 
double Ced_2331r_LNP = 0.
 
double Ced_2332i_LNP = 0.
 
double Ced_2332r_LNP = 0.
 
double Ced_2333i_LNP = 0.
 
double Ced_2333r_LNP = 0.
 
double Ced_3311r_LNP = 0.
 
double Ced_3312i_LNP = 0.
 
double Ced_3312r_LNP = 0.
 
double Ced_3313i_LNP = 0.
 
double Ced_3313r_LNP = 0.
 
double Ced_3322r_LNP = 0.
 
double Ced_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{ed})_{ijkm}\) (Imaginary part). More...
 
double Ced_3323r_LNP = 0.
 
double Ced_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{ed})_{ijkm}\) (Real part and pure real operator). More...
 
double Cee_1111r_LNP = 0.
 
double Cee_1112i_LNP = 0.
 
double Cee_1112r_LNP = 0.
 
double Cee_1113i_LNP = 0.
 
double Cee_1113r_LNP = 0.
 
double Cee_1122r_LNP = 0.
 
double Cee_1123i_LNP = 0.
 
double Cee_1123r_LNP = 0.
 
double Cee_1133r_LNP = 0.
 
double Cee_1212i_LNP = 0.
 
double Cee_1212r_LNP = 0.
 
double Cee_1213i_LNP = 0.
 
double Cee_1213r_LNP = 0.
 
double Cee_1222i_LNP = 0.
 
double Cee_1222r_LNP = 0.
 
double Cee_1223i_LNP = 0.
 
double Cee_1223r_LNP = 0.
 
double Cee_1232i_LNP = 0.
 
double Cee_1232r_LNP = 0.
 
double Cee_1233i_LNP = 0.
 
double Cee_1233r_LNP = 0.
 
double Cee_1313i_LNP = 0.
 
double Cee_1313r_LNP = 0.
 
double Cee_1323i_LNP = 0.
 
double Cee_1323r_LNP = 0.
 
double Cee_1333i_LNP = 0.
 
double Cee_1333r_LNP = 0.
 
double Cee_2222r_LNP = 0.
 
double Cee_2223i_LNP = 0.
 
double Cee_2223r_LNP = 0.
 
double Cee_2233r_LNP = 0.
 
double Cee_2323i_LNP = 0.
 
double Cee_2323r_LNP = 0.
 
double Cee_2333i_LNP = 0.
 The dimension-6 operator coefficient \((C_{ee})_{ijkm}\) (Imaginary part). More...
 
double Cee_2333r_LNP = 0.
 
double Cee_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{ee})_{ijkm}\) (Real part and pure real operator). More...
 
double CeH_11i_LNP = 0.
 
double CeH_11r_LNP = 0.
 
double CeH_12i_LNP = 0.
 
double CeH_12r_LNP = 0.
 
double CeH_13i_LNP = 0.
 
double CeH_13r_LNP = 0.
 
double CeH_21i_LNP = 0.
 
double CeH_21r_LNP = 0.
 
double CeH_22i_LNP = 0.
 
double CeH_22r_LNP = 0.
 
double CeH_23i_LNP = 0.
 
double CeH_23r_LNP = 0.
 
double CeH_31i_LNP = 0.
 
double CeH_31r_LNP = 0.
 
double CeH_32i_LNP = 0.
 
double CeH_32r_LNP = 0.
 
double CeH_33i_LNP = 0.
 The dimension-6 operator coefficient \((C_{eH})_{ij}\) (Imaginary part). More...
 
double CeH_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{eH})_{ij}\) (Real part and pure real operator). More...
 
double Ceu_1111r_LNP = 0.
 
double Ceu_1112i_LNP = 0.
 
double Ceu_1112r_LNP = 0.
 
double Ceu_1113i_LNP = 0.
 
double Ceu_1113r_LNP = 0.
 
double Ceu_1122r_LNP = 0.
 
double Ceu_1123i_LNP = 0.
 
double Ceu_1123r_LNP = 0.
 
double Ceu_1133r_LNP = 0.
 
double Ceu_1211i_LNP = 0.
 
double Ceu_1211r_LNP = 0.
 
double Ceu_1212i_LNP = 0.
 
double Ceu_1212r_LNP = 0.
 
double Ceu_1213i_LNP = 0.
 
double Ceu_1213r_LNP = 0.
 
double Ceu_1221i_LNP = 0.
 
double Ceu_1221r_LNP = 0.
 
double Ceu_1222i_LNP = 0.
 
double Ceu_1222r_LNP = 0.
 
double Ceu_1223i_LNP = 0.
 
double Ceu_1223r_LNP = 0.
 
double Ceu_1231i_LNP = 0.
 
double Ceu_1231r_LNP = 0.
 
double Ceu_1232i_LNP = 0.
 
double Ceu_1232r_LNP = 0.
 
double Ceu_1233i_LNP = 0.
 
double Ceu_1233r_LNP = 0.
 
double Ceu_1311i_LNP = 0.
 
double Ceu_1311r_LNP = 0.
 
double Ceu_1312i_LNP = 0.
 
double Ceu_1312r_LNP = 0.
 
double Ceu_1313i_LNP = 0.
 
double Ceu_1313r_LNP = 0.
 
double Ceu_1321i_LNP = 0.
 
double Ceu_1321r_LNP = 0.
 
double Ceu_1322i_LNP = 0.
 
double Ceu_1322r_LNP = 0.
 
double Ceu_1323i_LNP = 0.
 
double Ceu_1323r_LNP = 0.
 
double Ceu_1331i_LNP = 0.
 
double Ceu_1331r_LNP = 0.
 
double Ceu_1332i_LNP = 0.
 
double Ceu_1332r_LNP = 0.
 
double Ceu_1333i_LNP = 0.
 
double Ceu_1333r_LNP = 0.
 
double Ceu_2211r_LNP = 0.
 
double Ceu_2212i_LNP = 0.
 
double Ceu_2212r_LNP = 0.
 
double Ceu_2213i_LNP = 0.
 
double Ceu_2213r_LNP = 0.
 
double Ceu_2222r_LNP = 0.
 
double Ceu_2223i_LNP = 0.
 
double Ceu_2223r_LNP = 0.
 
double Ceu_2233r_LNP = 0.
 
double Ceu_2311i_LNP = 0.
 
double Ceu_2311r_LNP = 0.
 
double Ceu_2312i_LNP = 0.
 
double Ceu_2312r_LNP = 0.
 
double Ceu_2313i_LNP = 0.
 
double Ceu_2313r_LNP = 0.
 
double Ceu_2321i_LNP = 0.
 
double Ceu_2321r_LNP = 0.
 
double Ceu_2322i_LNP = 0.
 
double Ceu_2322r_LNP = 0.
 
double Ceu_2323i_LNP = 0.
 
double Ceu_2323r_LNP = 0.
 
double Ceu_2331i_LNP = 0.
 
double Ceu_2331r_LNP = 0.
 
double Ceu_2332i_LNP = 0.
 
double Ceu_2332r_LNP = 0.
 
double Ceu_2333i_LNP = 0.
 
double Ceu_2333r_LNP = 0.
 
double Ceu_3311r_LNP = 0.
 
double Ceu_3312i_LNP = 0.
 
double Ceu_3312r_LNP = 0.
 
double Ceu_3313i_LNP = 0.
 
double Ceu_3313r_LNP = 0.
 
double Ceu_3322r_LNP = 0.
 
double Ceu_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{eu})_{ijkm}\) (Imaginary part). More...
 
double Ceu_3323r_LNP = 0.
 
double Ceu_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{eu})_{ijkm}\) (Real part and pure real operator). More...
 
double CeW_11i_LNP = 0.
 
double CeW_11r_LNP = 0.
 
double CeW_12i_LNP = 0.
 
double CeW_12r_LNP = 0.
 
double CeW_13i_LNP = 0.
 
double CeW_13r_LNP = 0.
 
double CeW_21i_LNP = 0.
 
double CeW_21r_LNP = 0.
 
double CeW_22i_LNP = 0.
 
double CeW_22r_LNP = 0.
 
double CeW_23i_LNP = 0.
 
double CeW_23r_LNP = 0.
 
double CeW_31i_LNP = 0.
 
double CeW_31r_LNP = 0.
 
double CeW_32i_LNP = 0.
 
double CeW_32r_LNP = 0.
 
double CeW_33i_LNP = 0.
 The dimension-6 operator coefficient \((C_{eW})_{ij}\) (Imaginary part). More...
 
double CeW_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{eW})_{ij}\) (Real part and pure real operator). More...
 
double CG_LNP = 0.
 The dimension-6 operator coefficient \(C_{G}\). More...
 
double CGtilde_LNP = 0.
 The dimension-6 operator coefficient \(C_{\tilde{G}}\). More...
 
double CH_LNP = 0.
 The dimension-6 operator coefficient \(C_{H}\). More...
 
double CHB_LNP = 0.
 The dimension-6 operator coefficient \(C_{HB}\). More...
 
double CHbox_LNP = 0.
 The dimension-6 operator coefficient \(C_{H\Box}\). More...
 
double CHBtilde_LNP = 0.
 The dimension-6 operator coefficient \(C_{H\tilde{B}}\). More...
 
double CHd_11r_LNP = 0.
 
double CHd_12i_LNP = 0.
 
double CHd_12r_LNP = 0.
 
double CHd_13i_LNP = 0.
 
double CHd_13r_LNP = 0.
 
double CHd_22r_LNP = 0.
 
double CHd_23i_LNP = 0.
 The dimension-6 operator coefficient \((C_{Hd})_{ij}\) (Imaginary part). More...
 
double CHd_23r_LNP = 0.
 
double CHd_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{Hd})_{ij}\) (Real part and pure real operator). More...
 
double CHD_LNP = 0.
 The dimension-6 operator coefficient \(C_{HD}\). More...
 
double CHdEWbb = 0.
 CHd operators at the EW scale in the down-quark mass basis
More...
 
double CHdEWdd = 0.
 
double CHdEWss = 0.
 
double CHe_11r_LNP = 0.
 
double CHe_12i_LNP = 0.
 
double CHe_12r_LNP = 0.
 
double CHe_13i_LNP = 0.
 
double CHe_13r_LNP = 0.
 
double CHe_22r_LNP = 0.
 
double CHe_23i_LNP = 0.
 The dimension-6 operator coefficient \((C_{He})_{ij}\) (Imaginary part). More...
 
double CHe_23r_LNP = 0.
 
double CHe_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{He})_{ij}\) (Real part and pure real operator). More...
 
double CHG_LNP = 0.
 The dimension-6 operator coefficient \(C_{HG}\). More...
 
double CHGtilde_LNP = 0.
 The dimension-6 operator coefficient \(C_{H\tilde{G}}\). More...
 
double CHl1_11r_LNP = 0.
 
double CHl1_12i_LNP = 0.
 
double CHl1_12r_LNP = 0.
 
double CHl1_13i_LNP = 0.
 
double CHl1_13r_LNP = 0.
 
double CHl1_22r_LNP = 0.
 
double CHl1_23i_LNP = 0.
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{ij}\) (Imaginary part). More...
 
double CHl1_23r_LNP = 0.
 
double CHl1_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{HL}^{(1)})_{ij}\) (Real part and pure real operator). More...
 
double CHl3_11r_LNP = 0.
 
double CHl3_12i_LNP = 0.
 
double CHl3_12r_LNP = 0.
 
double CHl3_13i_LNP = 0.
 
double CHl3_13r_LNP = 0.
 
double CHl3_22r_LNP = 0.
 
double CHl3_23i_LNP = 0.
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{ij}\) (Imaginary part). More...
 
double CHl3_23r_LNP = 0.
 
double CHl3_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{HL}^{(3)})_{ij}\) (Real part and pure real operator). More...
 
double CHq1_11r_LNP = 0.
 
double CHq1_12i_LNP = 0.
 
double CHq1_12r_LNP = 0.
 
double CHq1_13i_LNP = 0.
 
double CHq1_13r_LNP = 0.
 
double CHq1_22r_LNP = 0.
 
double CHq1_23i_LNP = 0.
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{ij}\) (Imaginary part). More...
 
double CHq1_23r_LNP = 0.
 
double CHq1_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{ij}\) (Real part and pure real operator). More...
 
double CHq1EWbb = 0.
 CHq1 operators at the EW scale in the down-quark mass basis
More...
 
double CHq1EWcc = 0.
 
double CHq1EWdd = 0.
 
double CHq1EWss = 0.
 
double CHq1EWtt = 0.
 CHq1 operators at the EW scale in the up-quark mass basis. More...
 
double CHq1EWuu = 0.
 
double CHq3_11r_LNP = 0.
 
double CHq3_12i_LNP = 0.
 
double CHq3_12r_LNP = 0.
 
double CHq3_13i_LNP = 0.
 
double CHq3_13r_LNP = 0.
 
double CHq3_22r_LNP = 0.
 
double CHq3_23i_LNP = 0.
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{ij}\) (Imaginary part). More...
 
double CHq3_23r_LNP = 0.
 
double CHq3_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{ij}\) (Real part and pure real operator). More...
 
double CHq3EWbb = 0.
 CHq3 operators at the EW scale in the down-quark mass basis
More...
 
double CHq3EWcc = 0.
 
gslpp::complex CHq3EWcs = gslpp::complex(0., 0., false)
 
double CHq3EWdd = 0.
 
double CHq3EWss = 0.
 
gslpp::complex CHq3EWtb = gslpp::complex(0., 0., false)
 CHq3 operators at the EW scale in the up-down-quark mass basis
More...
 
double CHq3EWtt = 0.
 CHq3 operators at the EW scale in the up-quark mass basis. More...
 
gslpp::complex CHq3EWud = gslpp::complex(0., 0., false)
 
double CHq3EWuu = 0.
 
double cHSM
 Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes. More...
 
double CHu_11r_LNP = 0.
 
double CHu_12i_LNP = 0.
 
double CHu_12r_LNP = 0.
 
double CHu_13i_LNP = 0.
 
double CHu_13r_LNP = 0.
 
double CHu_22r_LNP = 0.
 
double CHu_23i_LNP = 0.
 The dimension-6 operator coefficient \((C_{Hu})_{ij}\) (Imaginary part). More...
 
double CHu_23r_LNP = 0.
 
double CHu_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{Hu})_{ij}\) (Real part and pure real operator). More...
 
double CHud_11i_LNP = 0.
 
double CHud_11r_LNP = 0.
 
double CHud_12i_LNP = 0.
 
double CHud_12r_LNP = 0.
 
double CHud_13i_LNP = 0.
 
double CHud_13r_LNP = 0.
 
double CHud_21i_LNP = 0.
 
double CHud_21r_LNP = 0.
 
double CHud_22i_LNP = 0.
 
double CHud_22r_LNP = 0.
 
double CHud_23i_LNP = 0.
 
double CHud_23r_LNP = 0.
 
double CHud_31i_LNP = 0.
 
double CHud_31r_LNP = 0.
 
double CHud_32i_LNP = 0.
 
double CHud_32r_LNP = 0.
 
double CHud_33i_LNP = 0.
 The dimension-6 operator coefficient \((C_{Hud})_{ij}\) (Imaginary part). More...
 
double CHud_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{Hud})_{ij}\) (Real part and pure real operator). More...
 
double CHuEWcc = 0.
 
double CHuEWtt = 0.
 CHu operators at the EW scale in the up-quark mass basis. More...
 
double CHuEWuu = 0.
 
double CHW_LNP = 0.
 The dimension-6 operator coefficient \(C_{HW}\). More...
 
double CHWB_LNP = 0.
 The dimension-6 operator coefficient \(C_{HWB}\). More...
 
double CHWtilde_LNP = 0.
 The dimension-6 operator coefficient \(C_{H\tilde{W}}\). More...
 
double CHWtildeB_LNP = 0.
 The dimension-6 operator coefficient \(C_{H\tilde{W}B}\). More...
 
double Cld_1111r_LNP = 0.
 
double Cld_1112i_LNP = 0.
 
double Cld_1112r_LNP = 0.
 
double Cld_1113i_LNP = 0.
 
double Cld_1113r_LNP = 0.
 
double Cld_1122r_LNP = 0.
 
double Cld_1123i_LNP = 0.
 
double Cld_1123r_LNP = 0.
 
double Cld_1133r_LNP = 0.
 
double Cld_1211i_LNP = 0.
 
double Cld_1211r_LNP = 0.
 
double Cld_1212i_LNP = 0.
 
double Cld_1212r_LNP = 0.
 
double Cld_1213i_LNP = 0.
 
double Cld_1213r_LNP = 0.
 
double Cld_1221i_LNP = 0.
 
double Cld_1221r_LNP = 0.
 
double Cld_1222i_LNP = 0.
 
double Cld_1222r_LNP = 0.
 
double Cld_1223i_LNP = 0.
 
double Cld_1223r_LNP = 0.
 
double Cld_1231i_LNP = 0.
 
double Cld_1231r_LNP = 0.
 
double Cld_1232i_LNP = 0.
 
double Cld_1232r_LNP = 0.
 
double Cld_1233i_LNP = 0.
 
double Cld_1233r_LNP = 0.
 
double Cld_1311i_LNP = 0.
 
double Cld_1311r_LNP = 0.
 
double Cld_1312i_LNP = 0.
 
double Cld_1312r_LNP = 0.
 
double Cld_1313i_LNP = 0.
 
double Cld_1313r_LNP = 0.
 
double Cld_1321i_LNP = 0.
 
double Cld_1321r_LNP = 0.
 
double Cld_1322i_LNP = 0.
 
double Cld_1322r_LNP = 0.
 
double Cld_1323i_LNP = 0.
 
double Cld_1323r_LNP = 0.
 
double Cld_1331i_LNP = 0.
 
double Cld_1331r_LNP = 0.
 
double Cld_1332i_LNP = 0.
 
double Cld_1332r_LNP = 0.
 
double Cld_1333i_LNP = 0.
 
double Cld_1333r_LNP = 0.
 
double Cld_2211r_LNP = 0.
 
double Cld_2212i_LNP = 0.
 
double Cld_2212r_LNP = 0.
 
double Cld_2213i_LNP = 0.
 
double Cld_2213r_LNP = 0.
 
double Cld_2222r_LNP = 0.
 
double Cld_2223i_LNP = 0.
 
double Cld_2223r_LNP = 0.
 
double Cld_2233r_LNP = 0.
 
double Cld_2311i_LNP = 0.
 
double Cld_2311r_LNP = 0.
 
double Cld_2312i_LNP = 0.
 
double Cld_2312r_LNP = 0.
 
double Cld_2313i_LNP = 0.
 
double Cld_2313r_LNP = 0.
 
double Cld_2321i_LNP = 0.
 
double Cld_2321r_LNP = 0.
 
double Cld_2322i_LNP = 0.
 
double Cld_2322r_LNP = 0.
 
double Cld_2323i_LNP = 0.
 
double Cld_2323r_LNP = 0.
 
double Cld_2331i_LNP = 0.
 
double Cld_2331r_LNP = 0.
 
double Cld_2332i_LNP = 0.
 
double Cld_2332r_LNP = 0.
 
double Cld_2333i_LNP = 0.
 
double Cld_2333r_LNP = 0.
 
double Cld_3311r_LNP = 0.
 
double Cld_3312i_LNP = 0.
 
double Cld_3312r_LNP = 0.
 
double Cld_3313i_LNP = 0.
 
double Cld_3313r_LNP = 0.
 
double Cld_3322r_LNP = 0.
 
double Cld_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{ld})_{ijkm}\) (Imaginary part). More...
 
double Cld_3323r_LNP = 0.
 
double Cld_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{ld})_{ijkm}\) (Real part and pure real operator). More...
 
double Cle_1111r_LNP = 0.
 
double Cle_1112i_LNP = 0.
 
double Cle_1112r_LNP = 0.
 
double Cle_1113i_LNP = 0.
 
double Cle_1113r_LNP = 0.
 
double Cle_1122r_LNP = 0.
 
double Cle_1123i_LNP = 0.
 
double Cle_1123r_LNP = 0.
 
double Cle_1133r_LNP = 0.
 
double Cle_1211i_LNP = 0.
 
double Cle_1211r_LNP = 0.
 
double Cle_1212i_LNP = 0.
 
double Cle_1212r_LNP = 0.
 
double Cle_1213i_LNP = 0.
 
double Cle_1213r_LNP = 0.
 
double Cle_1221i_LNP = 0.
 
double Cle_1221r_LNP = 0.
 
double Cle_1222i_LNP = 0.
 
double Cle_1222r_LNP = 0.
 
double Cle_1223i_LNP = 0.
 
double Cle_1223r_LNP = 0.
 
double Cle_1231i_LNP = 0.
 
double Cle_1231r_LNP = 0.
 
double Cle_1232i_LNP = 0.
 
double Cle_1232r_LNP = 0.
 
double Cle_1233i_LNP = 0.
 
double Cle_1233r_LNP = 0.
 
double Cle_1311i_LNP = 0.
 
double Cle_1311r_LNP = 0.
 
double Cle_1312i_LNP = 0.
 
double Cle_1312r_LNP = 0.
 
double Cle_1313i_LNP = 0.
 
double Cle_1313r_LNP = 0.
 
double Cle_1321i_LNP = 0.
 
double Cle_1321r_LNP = 0.
 
double Cle_1322i_LNP = 0.
 
double Cle_1322r_LNP = 0.
 
double Cle_1323i_LNP = 0.
 
double Cle_1323r_LNP = 0.
 
double Cle_1331i_LNP = 0.
 
double Cle_1331r_LNP = 0.
 
double Cle_1332i_LNP = 0.
 
double Cle_1332r_LNP = 0.
 
double Cle_1333i_LNP = 0.
 
double Cle_1333r_LNP = 0.
 
double Cle_2211r_LNP = 0.
 
double Cle_2212i_LNP = 0.
 
double Cle_2212r_LNP = 0.
 
double Cle_2213i_LNP = 0.
 
double Cle_2213r_LNP = 0.
 
double Cle_2222r_LNP = 0.
 
double Cle_2223i_LNP = 0.
 
double Cle_2223r_LNP = 0.
 
double Cle_2233r_LNP = 0.
 
double Cle_2311i_LNP = 0.
 
double Cle_2311r_LNP = 0.
 
double Cle_2312i_LNP = 0.
 
double Cle_2312r_LNP = 0.
 
double Cle_2313i_LNP = 0.
 
double Cle_2313r_LNP = 0.
 
double Cle_2321i_LNP = 0.
 
double Cle_2321r_LNP = 0.
 
double Cle_2322i_LNP = 0.
 
double Cle_2322r_LNP = 0.
 
double Cle_2323i_LNP = 0.
 
double Cle_2323r_LNP = 0.
 
double Cle_2331i_LNP = 0.
 
double Cle_2331r_LNP = 0.
 
double Cle_2332i_LNP = 0.
 
double Cle_2332r_LNP = 0.
 
double Cle_2333i_LNP = 0.
 
double Cle_2333r_LNP = 0.
 
double Cle_3311r_LNP = 0.
 
double Cle_3312i_LNP = 0.
 
double Cle_3312r_LNP = 0.
 
double Cle_3313i_LNP = 0.
 
double Cle_3313r_LNP = 0.
 
double Cle_3322r_LNP = 0.
 
double Cle_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{le})_{ijkm}\) (Imaginary part). More...
 
double Cle_3323r_LNP = 0.
 
double Cle_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{le})_{ijkm}\) (Real part and pure real operator). More...
 
double Cledq_1111i_LNP = 0.
 
double Cledq_1111r_LNP = 0.
 
double Cledq_1112i_LNP = 0.
 
double Cledq_1112r_LNP = 0.
 
double Cledq_1113i_LNP = 0.
 
double Cledq_1113r_LNP = 0.
 
double Cledq_1121i_LNP = 0.
 
double Cledq_1121r_LNP = 0.
 
double Cledq_1122i_LNP = 0.
 
double Cledq_1122r_LNP = 0.
 
double Cledq_1123i_LNP = 0.
 
double Cledq_1123r_LNP = 0.
 
double Cledq_1131i_LNP = 0.
 
double Cledq_1131r_LNP = 0.
 
double Cledq_1132i_LNP = 0.
 
double Cledq_1132r_LNP = 0.
 
double Cledq_1133i_LNP = 0.
 
double Cledq_1133r_LNP = 0.
 
double Cledq_1211i_LNP = 0.
 
double Cledq_1211r_LNP = 0.
 
double Cledq_1212i_LNP = 0.
 
double Cledq_1212r_LNP = 0.
 
double Cledq_1213i_LNP = 0.
 
double Cledq_1213r_LNP = 0.
 
double Cledq_1221i_LNP = 0.
 
double Cledq_1221r_LNP = 0.
 
double Cledq_1222i_LNP = 0.
 
double Cledq_1222r_LNP = 0.
 
double Cledq_1223i_LNP = 0.
 
double Cledq_1223r_LNP = 0.
 
double Cledq_1231i_LNP = 0.
 
double Cledq_1231r_LNP = 0.
 
double Cledq_1232i_LNP = 0.
 
double Cledq_1232r_LNP = 0.
 
double Cledq_1233i_LNP = 0.
 
double Cledq_1233r_LNP = 0.
 
double Cledq_1311i_LNP = 0.
 
double Cledq_1311r_LNP = 0.
 
double Cledq_1312i_LNP = 0.
 
double Cledq_1312r_LNP = 0.
 
double Cledq_1313i_LNP = 0.
 
double Cledq_1313r_LNP = 0.
 
double Cledq_1321i_LNP = 0.
 
double Cledq_1321r_LNP = 0.
 
double Cledq_1322i_LNP = 0.
 
double Cledq_1322r_LNP = 0.
 
double Cledq_1323i_LNP = 0.
 
double Cledq_1323r_LNP = 0.
 
double Cledq_1331i_LNP = 0.
 
double Cledq_1331r_LNP = 0.
 
double Cledq_1332i_LNP = 0.
 
double Cledq_1332r_LNP = 0.
 
double Cledq_1333i_LNP = 0.
 
double Cledq_1333r_LNP = 0.
 
double Cledq_2111i_LNP = 0.
 
double Cledq_2111r_LNP = 0.
 
double Cledq_2112i_LNP = 0.
 
double Cledq_2112r_LNP = 0.
 
double Cledq_2113i_LNP = 0.
 
double Cledq_2113r_LNP = 0.
 
double Cledq_2121i_LNP = 0.
 
double Cledq_2121r_LNP = 0.
 
double Cledq_2122i_LNP = 0.
 
double Cledq_2122r_LNP = 0.
 
double Cledq_2123i_LNP = 0.
 
double Cledq_2123r_LNP = 0.
 
double Cledq_2131i_LNP = 0.
 
double Cledq_2131r_LNP = 0.
 
double Cledq_2132i_LNP = 0.
 
double Cledq_2132r_LNP = 0.
 
double Cledq_2133i_LNP = 0.
 
double Cledq_2133r_LNP = 0.
 
double Cledq_2211i_LNP = 0.
 
double Cledq_2211r_LNP = 0.
 
double Cledq_2212i_LNP = 0.
 
double Cledq_2212r_LNP = 0.
 
double Cledq_2213i_LNP = 0.
 
double Cledq_2213r_LNP = 0.
 
double Cledq_2221i_LNP = 0.
 
double Cledq_2221r_LNP = 0.
 
double Cledq_2222i_LNP = 0.
 
double Cledq_2222r_LNP = 0.
 
double Cledq_2223i_LNP = 0.
 
double Cledq_2223r_LNP = 0.
 
double Cledq_2231i_LNP = 0.
 
double Cledq_2231r_LNP = 0.
 
double Cledq_2232i_LNP = 0.
 
double Cledq_2232r_LNP = 0.
 
double Cledq_2233i_LNP = 0.
 
double Cledq_2233r_LNP = 0.
 
double Cledq_2311i_LNP = 0.
 
double Cledq_2311r_LNP = 0.
 
double Cledq_2312i_LNP = 0.
 
double Cledq_2312r_LNP = 0.
 
double Cledq_2313i_LNP = 0.
 
double Cledq_2313r_LNP = 0.
 
double Cledq_2321i_LNP = 0.
 
double Cledq_2321r_LNP = 0.
 
double Cledq_2322i_LNP = 0.
 
double Cledq_2322r_LNP = 0.
 
double Cledq_2323i_LNP = 0.
 
double Cledq_2323r_LNP = 0.
 
double Cledq_2331i_LNP = 0.
 
double Cledq_2331r_LNP = 0.
 
double Cledq_2332i_LNP = 0.
 
double Cledq_2332r_LNP = 0.
 
double Cledq_2333i_LNP = 0.
 
double Cledq_2333r_LNP = 0.
 
double Cledq_3111i_LNP = 0.
 
double Cledq_3111r_LNP = 0.
 
double Cledq_3112i_LNP = 0.
 
double Cledq_3112r_LNP = 0.
 
double Cledq_3113i_LNP = 0.
 
double Cledq_3113r_LNP = 0.
 
double Cledq_3121i_LNP = 0.
 
double Cledq_3121r_LNP = 0.
 
double Cledq_3122i_LNP = 0.
 
double Cledq_3122r_LNP = 0.
 
double Cledq_3123i_LNP = 0.
 
double Cledq_3123r_LNP = 0.
 
double Cledq_3131i_LNP = 0.
 
double Cledq_3131r_LNP = 0.
 
double Cledq_3132i_LNP = 0.
 
double Cledq_3132r_LNP = 0.
 
double Cledq_3133i_LNP = 0.
 
double Cledq_3133r_LNP = 0.
 
double Cledq_3211i_LNP = 0.
 
double Cledq_3211r_LNP = 0.
 
double Cledq_3212i_LNP = 0.
 
double Cledq_3212r_LNP = 0.
 
double Cledq_3213i_LNP = 0.
 
double Cledq_3213r_LNP = 0.
 
double Cledq_3221i_LNP = 0.
 
double Cledq_3221r_LNP = 0.
 
double Cledq_3222i_LNP = 0.
 
double Cledq_3222r_LNP = 0.
 
double Cledq_3223i_LNP = 0.
 
double Cledq_3223r_LNP = 0.
 
double Cledq_3231i_LNP = 0.
 
double Cledq_3231r_LNP = 0.
 
double Cledq_3232i_LNP = 0.
 
double Cledq_3232r_LNP = 0.
 
double Cledq_3233i_LNP = 0.
 
double Cledq_3233r_LNP = 0.
 
double Cledq_3311i_LNP = 0.
 
double Cledq_3311r_LNP = 0.
 
double Cledq_3312i_LNP = 0.
 
double Cledq_3312r_LNP = 0.
 
double Cledq_3313i_LNP = 0.
 
double Cledq_3313r_LNP = 0.
 
double Cledq_3321i_LNP = 0.
 
double Cledq_3321r_LNP = 0.
 
double Cledq_3322i_LNP = 0.
 
double Cledq_3322r_LNP = 0.
 
double Cledq_3323i_LNP = 0.
 
double Cledq_3323r_LNP = 0.
 
double Cledq_3331i_LNP = 0.
 
double Cledq_3331r_LNP = 0.
 
double Cledq_3332i_LNP = 0.
 
double Cledq_3332r_LNP = 0.
 
double Cledq_3333i_LNP = 0.
 The dimension-6 operator coefficient \((C_{ledq})_{ijkm}\) (Imaginary part). More...
 
double Cledq_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{ledq})_{ijkm}\) (Real part and pure real operator). More...
 
double Clequ1_1111i_LNP = 0.
 
double Clequ1_1111r_LNP = 0.
 
double Clequ1_1112i_LNP = 0.
 
double Clequ1_1112r_LNP = 0.
 
double Clequ1_1113i_LNP = 0.
 
double Clequ1_1113r_LNP = 0.
 
double Clequ1_1121i_LNP = 0.
 
double Clequ1_1121r_LNP = 0.
 
double Clequ1_1122i_LNP = 0.
 
double Clequ1_1122r_LNP = 0.
 
double Clequ1_1123i_LNP = 0.
 
double Clequ1_1123r_LNP = 0.
 
double Clequ1_1131i_LNP = 0.
 
double Clequ1_1131r_LNP = 0.
 
double Clequ1_1132i_LNP = 0.
 
double Clequ1_1132r_LNP = 0.
 
double Clequ1_1133i_LNP = 0.
 
double Clequ1_1133r_LNP = 0.
 
double Clequ1_1211i_LNP = 0.
 
double Clequ1_1211r_LNP = 0.
 
double Clequ1_1212i_LNP = 0.
 
double Clequ1_1212r_LNP = 0.
 
double Clequ1_1213i_LNP = 0.
 
double Clequ1_1213r_LNP = 0.
 
double Clequ1_1221i_LNP = 0.
 
double Clequ1_1221r_LNP = 0.
 
double Clequ1_1222i_LNP = 0.
 
double Clequ1_1222r_LNP = 0.
 
double Clequ1_1223i_LNP = 0.
 
double Clequ1_1223r_LNP = 0.
 
double Clequ1_1231i_LNP = 0.
 
double Clequ1_1231r_LNP = 0.
 
double Clequ1_1232i_LNP = 0.
 
double Clequ1_1232r_LNP = 0.
 
double Clequ1_1233i_LNP = 0.
 
double Clequ1_1233r_LNP = 0.
 
double Clequ1_1311i_LNP = 0.
 
double Clequ1_1311r_LNP = 0.
 
double Clequ1_1312i_LNP = 0.
 
double Clequ1_1312r_LNP = 0.
 
double Clequ1_1313i_LNP = 0.
 
double Clequ1_1313r_LNP = 0.
 
double Clequ1_1321i_LNP = 0.
 
double Clequ1_1321r_LNP = 0.
 
double Clequ1_1322i_LNP = 0.
 
double Clequ1_1322r_LNP = 0.
 
double Clequ1_1323i_LNP = 0.
 
double Clequ1_1323r_LNP = 0.
 
double Clequ1_1331i_LNP = 0.
 
double Clequ1_1331r_LNP = 0.
 
double Clequ1_1332i_LNP = 0.
 
double Clequ1_1332r_LNP = 0.
 
double Clequ1_1333i_LNP = 0.
 
double Clequ1_1333r_LNP = 0.
 
double Clequ1_2111i_LNP = 0.
 
double Clequ1_2111r_LNP = 0.
 
double Clequ1_2112i_LNP = 0.
 
double Clequ1_2112r_LNP = 0.
 
double Clequ1_2113i_LNP = 0.
 
double Clequ1_2113r_LNP = 0.
 
double Clequ1_2121i_LNP = 0.
 
double Clequ1_2121r_LNP = 0.
 
double Clequ1_2122i_LNP = 0.
 
double Clequ1_2122r_LNP = 0.
 
double Clequ1_2123i_LNP = 0.
 
double Clequ1_2123r_LNP = 0.
 
double Clequ1_2131i_LNP = 0.
 
double Clequ1_2131r_LNP = 0.
 
double Clequ1_2132i_LNP = 0.
 
double Clequ1_2132r_LNP = 0.
 
double Clequ1_2133i_LNP = 0.
 
double Clequ1_2133r_LNP = 0.
 
double Clequ1_2211i_LNP = 0.
 
double Clequ1_2211r_LNP = 0.
 
double Clequ1_2212i_LNP = 0.
 
double Clequ1_2212r_LNP = 0.
 
double Clequ1_2213i_LNP = 0.
 
double Clequ1_2213r_LNP = 0.
 
double Clequ1_2221i_LNP = 0.
 
double Clequ1_2221r_LNP = 0.
 
double Clequ1_2222i_LNP = 0.
 
double Clequ1_2222r_LNP = 0.
 
double Clequ1_2223i_LNP = 0.
 
double Clequ1_2223r_LNP = 0.
 
double Clequ1_2231i_LNP = 0.
 
double Clequ1_2231r_LNP = 0.
 
double Clequ1_2232i_LNP = 0.
 
double Clequ1_2232r_LNP = 0.
 
double Clequ1_2233i_LNP = 0.
 
double Clequ1_2233r_LNP = 0.
 
double Clequ1_2311i_LNP = 0.
 
double Clequ1_2311r_LNP = 0.
 
double Clequ1_2312i_LNP = 0.
 
double Clequ1_2312r_LNP = 0.
 
double Clequ1_2313i_LNP = 0.
 
double Clequ1_2313r_LNP = 0.
 
double Clequ1_2321i_LNP = 0.
 
double Clequ1_2321r_LNP = 0.
 
double Clequ1_2322i_LNP = 0.
 
double Clequ1_2322r_LNP = 0.
 
double Clequ1_2323i_LNP = 0.
 
double Clequ1_2323r_LNP = 0.
 
double Clequ1_2331i_LNP = 0.
 
double Clequ1_2331r_LNP = 0.
 
double Clequ1_2332i_LNP = 0.
 
double Clequ1_2332r_LNP = 0.
 
double Clequ1_2333i_LNP = 0.
 
double Clequ1_2333r_LNP = 0.
 
double Clequ1_3111i_LNP = 0.
 
double Clequ1_3111r_LNP = 0.
 
double Clequ1_3112i_LNP = 0.
 
double Clequ1_3112r_LNP = 0.
 
double Clequ1_3113i_LNP = 0.
 
double Clequ1_3113r_LNP = 0.
 
double Clequ1_3121i_LNP = 0.
 
double Clequ1_3121r_LNP = 0.
 
double Clequ1_3122i_LNP = 0.
 
double Clequ1_3122r_LNP = 0.
 
double Clequ1_3123i_LNP = 0.
 
double Clequ1_3123r_LNP = 0.
 
double Clequ1_3131i_LNP = 0.
 
double Clequ1_3131r_LNP = 0.
 
double Clequ1_3132i_LNP = 0.
 
double Clequ1_3132r_LNP = 0.
 
double Clequ1_3133i_LNP = 0.
 
double Clequ1_3133r_LNP = 0.
 
double Clequ1_3211i_LNP = 0.
 
double Clequ1_3211r_LNP = 0.
 
double Clequ1_3212i_LNP = 0.
 
double Clequ1_3212r_LNP = 0.
 
double Clequ1_3213i_LNP = 0.
 
double Clequ1_3213r_LNP = 0.
 
double Clequ1_3221i_LNP = 0.
 
double Clequ1_3221r_LNP = 0.
 
double Clequ1_3222i_LNP = 0.
 
double Clequ1_3222r_LNP = 0.
 
double Clequ1_3223i_LNP = 0.
 
double Clequ1_3223r_LNP = 0.
 
double Clequ1_3231i_LNP = 0.
 
double Clequ1_3231r_LNP = 0.
 
double Clequ1_3232i_LNP = 0.
 
double Clequ1_3232r_LNP = 0.
 
double Clequ1_3233i_LNP = 0.
 
double Clequ1_3233r_LNP = 0.
 
double Clequ1_3311i_LNP = 0.
 
double Clequ1_3311r_LNP = 0.
 
double Clequ1_3312i_LNP = 0.
 
double Clequ1_3312r_LNP = 0.
 
double Clequ1_3313i_LNP = 0.
 
double Clequ1_3313r_LNP = 0.
 
double Clequ1_3321i_LNP = 0.
 
double Clequ1_3321r_LNP = 0.
 
double Clequ1_3322i_LNP = 0.
 
double Clequ1_3322r_LNP = 0.
 
double Clequ1_3323i_LNP = 0.
 
double Clequ1_3323r_LNP = 0.
 
double Clequ1_3331i_LNP = 0.
 
double Clequ1_3331r_LNP = 0.
 
double Clequ1_3332i_LNP = 0.
 
double Clequ1_3332r_LNP = 0.
 
double Clequ1_3333i_LNP = 0.
 The dimension-6 operator coefficient \((C_{lequ}^{(1)})_{ijkm}\) (Imaginary part). More...
 
double Clequ1_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{lequ}^{(1)})_{ijkm}\) (Real part and pure real operator). More...
 
double Clequ3_1111i_LNP = 0.
 
double Clequ3_1111r_LNP = 0.
 
double Clequ3_1112i_LNP = 0.
 
double Clequ3_1112r_LNP = 0.
 
double Clequ3_1113i_LNP = 0.
 
double Clequ3_1113r_LNP = 0.
 
double Clequ3_1121i_LNP = 0.
 
double Clequ3_1121r_LNP = 0.
 
double Clequ3_1122i_LNP = 0.
 
double Clequ3_1122r_LNP = 0.
 
double Clequ3_1123i_LNP = 0.
 
double Clequ3_1123r_LNP = 0.
 
double Clequ3_1131i_LNP = 0.
 
double Clequ3_1131r_LNP = 0.
 
double Clequ3_1132i_LNP = 0.
 
double Clequ3_1132r_LNP = 0.
 
double Clequ3_1133i_LNP = 0.
 
double Clequ3_1133r_LNP = 0.
 
double Clequ3_1211i_LNP = 0.
 
double Clequ3_1211r_LNP = 0.
 
double Clequ3_1212i_LNP = 0.
 
double Clequ3_1212r_LNP = 0.
 
double Clequ3_1213i_LNP = 0.
 
double Clequ3_1213r_LNP = 0.
 
double Clequ3_1221i_LNP = 0.
 
double Clequ3_1221r_LNP = 0.
 
double Clequ3_1222i_LNP = 0.
 
double Clequ3_1222r_LNP = 0.
 
double Clequ3_1223i_LNP = 0.
 
double Clequ3_1223r_LNP = 0.
 
double Clequ3_1231i_LNP = 0.
 
double Clequ3_1231r_LNP = 0.
 
double Clequ3_1232i_LNP = 0.
 
double Clequ3_1232r_LNP = 0.
 
double Clequ3_1233i_LNP = 0.
 
double Clequ3_1233r_LNP = 0.
 
double Clequ3_1311i_LNP = 0.
 
double Clequ3_1311r_LNP = 0.
 
double Clequ3_1312i_LNP = 0.
 
double Clequ3_1312r_LNP = 0.
 
double Clequ3_1313i_LNP = 0.
 
double Clequ3_1313r_LNP = 0.
 
double Clequ3_1321i_LNP = 0.
 
double Clequ3_1321r_LNP = 0.
 
double Clequ3_1322i_LNP = 0.
 
double Clequ3_1322r_LNP = 0.
 
double Clequ3_1323i_LNP = 0.
 
double Clequ3_1323r_LNP = 0.
 
double Clequ3_1331i_LNP = 0.
 
double Clequ3_1331r_LNP = 0.
 
double Clequ3_1332i_LNP = 0.
 
double Clequ3_1332r_LNP = 0.
 
double Clequ3_1333i_LNP = 0.
 
double Clequ3_1333r_LNP = 0.
 
double Clequ3_2111i_LNP = 0.
 
double Clequ3_2111r_LNP = 0.
 
double Clequ3_2112i_LNP = 0.
 
double Clequ3_2112r_LNP = 0.
 
double Clequ3_2113i_LNP = 0.
 
double Clequ3_2113r_LNP = 0.
 
double Clequ3_2121i_LNP = 0.
 
double Clequ3_2121r_LNP = 0.
 
double Clequ3_2122i_LNP = 0.
 
double Clequ3_2122r_LNP = 0.
 
double Clequ3_2123i_LNP = 0.
 
double Clequ3_2123r_LNP = 0.
 
double Clequ3_2131i_LNP = 0.
 
double Clequ3_2131r_LNP = 0.
 
double Clequ3_2132i_LNP = 0.
 
double Clequ3_2132r_LNP = 0.
 
double Clequ3_2133i_LNP = 0.
 
double Clequ3_2133r_LNP = 0.
 
double Clequ3_2211i_LNP = 0.
 
double Clequ3_2211r_LNP = 0.
 
double Clequ3_2212i_LNP = 0.
 
double Clequ3_2212r_LNP = 0.
 
double Clequ3_2213i_LNP = 0.
 
double Clequ3_2213r_LNP = 0.
 
double Clequ3_2221i_LNP = 0.
 
double Clequ3_2221r_LNP = 0.
 
double Clequ3_2222i_LNP = 0.
 
double Clequ3_2222r_LNP = 0.
 
double Clequ3_2223i_LNP = 0.
 
double Clequ3_2223r_LNP = 0.
 
double Clequ3_2231i_LNP = 0.
 
double Clequ3_2231r_LNP = 0.
 
double Clequ3_2232i_LNP = 0.
 
double Clequ3_2232r_LNP = 0.
 
double Clequ3_2233i_LNP = 0.
 
double Clequ3_2233r_LNP = 0.
 
double Clequ3_2311i_LNP = 0.
 
double Clequ3_2311r_LNP = 0.
 
double Clequ3_2312i_LNP = 0.
 
double Clequ3_2312r_LNP = 0.
 
double Clequ3_2313i_LNP = 0.
 
double Clequ3_2313r_LNP = 0.
 
double Clequ3_2321i_LNP = 0.
 
double Clequ3_2321r_LNP = 0.
 
double Clequ3_2322i_LNP = 0.
 
double Clequ3_2322r_LNP = 0.
 
double Clequ3_2323i_LNP = 0.
 
double Clequ3_2323r_LNP = 0.
 
double Clequ3_2331i_LNP = 0.
 
double Clequ3_2331r_LNP = 0.
 
double Clequ3_2332i_LNP = 0.
 
double Clequ3_2332r_LNP = 0.
 
double Clequ3_2333i_LNP = 0.
 
double Clequ3_2333r_LNP = 0.
 
double Clequ3_3111i_LNP = 0.
 
double Clequ3_3111r_LNP = 0.
 
double Clequ3_3112i_LNP = 0.
 
double Clequ3_3112r_LNP = 0.
 
double Clequ3_3113i_LNP = 0.
 
double Clequ3_3113r_LNP = 0.
 
double Clequ3_3121i_LNP = 0.
 
double Clequ3_3121r_LNP = 0.
 
double Clequ3_3122i_LNP = 0.
 
double Clequ3_3122r_LNP = 0.
 
double Clequ3_3123i_LNP = 0.
 
double Clequ3_3123r_LNP = 0.
 
double Clequ3_3131i_LNP = 0.
 
double Clequ3_3131r_LNP = 0.
 
double Clequ3_3132i_LNP = 0.
 
double Clequ3_3132r_LNP = 0.
 
double Clequ3_3133i_LNP = 0.
 
double Clequ3_3133r_LNP = 0.
 
double Clequ3_3211i_LNP = 0.
 
double Clequ3_3211r_LNP = 0.
 
double Clequ3_3212i_LNP = 0.
 
double Clequ3_3212r_LNP = 0.
 
double Clequ3_3213i_LNP = 0.
 
double Clequ3_3213r_LNP = 0.
 
double Clequ3_3221i_LNP = 0.
 
double Clequ3_3221r_LNP = 0.
 
double Clequ3_3222i_LNP = 0.
 
double Clequ3_3222r_LNP = 0.
 
double Clequ3_3223i_LNP = 0.
 
double Clequ3_3223r_LNP = 0.
 
double Clequ3_3231i_LNP = 0.
 
double Clequ3_3231r_LNP = 0.
 
double Clequ3_3232i_LNP = 0.
 
double Clequ3_3232r_LNP = 0.
 
double Clequ3_3233i_LNP = 0.
 
double Clequ3_3233r_LNP = 0.
 
double Clequ3_3311i_LNP = 0.
 
double Clequ3_3311r_LNP = 0.
 
double Clequ3_3312i_LNP = 0.
 
double Clequ3_3312r_LNP = 0.
 
double Clequ3_3313i_LNP = 0.
 
double Clequ3_3313r_LNP = 0.
 
double Clequ3_3321i_LNP = 0.
 
double Clequ3_3321r_LNP = 0.
 
double Clequ3_3322i_LNP = 0.
 
double Clequ3_3322r_LNP = 0.
 
double Clequ3_3323i_LNP = 0.
 
double Clequ3_3323r_LNP = 0.
 
double Clequ3_3331i_LNP = 0.
 
double Clequ3_3331r_LNP = 0.
 
double Clequ3_3332i_LNP = 0.
 
double Clequ3_3332r_LNP = 0.
 
double Clequ3_3333i_LNP = 0.
 The dimension-6 operator coefficient \((C_{lequ}^{(3)})_{ijkm}\) (Imaginary part). More...
 
double Clequ3_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{lequ}^{(3)})_{ijkm}\) (Real part and pure real operator). More...
 
double cLH3d62
 Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms). More...
 
double cLHd6
 Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions. More...
 
double Cll_1111r_LNP = 0.
 
double Cll_1112i_LNP = 0.
 
double Cll_1112r_LNP = 0.
 
double Cll_1113i_LNP = 0.
 
double Cll_1113r_LNP = 0.
 
double Cll_1122r_LNP = 0.
 
double Cll_1123i_LNP = 0.
 
double Cll_1123r_LNP = 0.
 
double Cll_1133r_LNP = 0.
 
double Cll_1212i_LNP = 0.
 
double Cll_1212r_LNP = 0.
 
double Cll_1213i_LNP = 0.
 
double Cll_1213r_LNP = 0.
 
double Cll_1221r_LNP = 0.
 
double Cll_1222i_LNP = 0.
 
double Cll_1222r_LNP = 0.
 
double Cll_1223i_LNP = 0.
 
double Cll_1223r_LNP = 0.
 
double Cll_1231i_LNP = 0.
 
double Cll_1231r_LNP = 0.
 
double Cll_1232i_LNP = 0.
 
double Cll_1232r_LNP = 0.
 
double Cll_1233i_LNP = 0.
 
double Cll_1233r_LNP = 0.
 
double Cll_1313i_LNP = 0.
 
double Cll_1313r_LNP = 0.
 
double Cll_1322i_LNP = 0.
 
double Cll_1322r_LNP = 0.
 
double Cll_1323i_LNP = 0.
 
double Cll_1323r_LNP = 0.
 
double Cll_1331r_LNP = 0.
 
double Cll_1332i_LNP = 0.
 
double Cll_1332r_LNP = 0.
 
double Cll_1333i_LNP = 0.
 
double Cll_1333r_LNP = 0.
 
double Cll_2222r_LNP = 0.
 
double Cll_2223i_LNP = 0.
 
double Cll_2223r_LNP = 0.
 
double Cll_2233r_LNP = 0.
 
double Cll_2323i_LNP = 0.
 
double Cll_2323r_LNP = 0.
 
double Cll_2332r_LNP = 0.
 
double Cll_2333i_LNP = 0.
 The dimension-6 operator coefficient \((C_{ll})_{ijkm}\) (Imaginary part). More...
 
double Cll_2333r_LNP = 0.
 
double Cll_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{ll})_{ijkm}\) (Real part and pure real operator). More...
 
double Clq1_1111r_LNP = 0.
 
double Clq1_1112i_LNP = 0.
 
double Clq1_1112r_LNP = 0.
 
double Clq1_1113i_LNP = 0.
 
double Clq1_1113r_LNP = 0.
 
double Clq1_1122r_LNP = 0.
 
double Clq1_1123i_LNP = 0.
 
double Clq1_1123r_LNP = 0.
 
double Clq1_1133r_LNP = 0.
 
double Clq1_1211i_LNP = 0.
 
double Clq1_1211r_LNP = 0.
 
double Clq1_1212i_LNP = 0.
 
double Clq1_1212r_LNP = 0.
 
double Clq1_1213i_LNP = 0.
 
double Clq1_1213r_LNP = 0.
 
double Clq1_1221i_LNP = 0.
 
double Clq1_1221r_LNP = 0.
 
double Clq1_1222i_LNP = 0.
 
double Clq1_1222r_LNP = 0.
 
double Clq1_1223i_LNP = 0.
 
double Clq1_1223r_LNP = 0.
 
double Clq1_1231i_LNP = 0.
 
double Clq1_1231r_LNP = 0.
 
double Clq1_1232i_LNP = 0.
 
double Clq1_1232r_LNP = 0.
 
double Clq1_1233i_LNP = 0.
 
double Clq1_1233r_LNP = 0.
 
double Clq1_1311i_LNP = 0.
 
double Clq1_1311r_LNP = 0.
 
double Clq1_1312i_LNP = 0.
 
double Clq1_1312r_LNP = 0.
 
double Clq1_1313i_LNP = 0.
 
double Clq1_1313r_LNP = 0.
 
double Clq1_1321i_LNP = 0.
 
double Clq1_1321r_LNP = 0.
 
double Clq1_1322i_LNP = 0.
 
double Clq1_1322r_LNP = 0.
 
double Clq1_1323i_LNP = 0.
 
double Clq1_1323r_LNP = 0.
 
double Clq1_1331i_LNP = 0.
 
double Clq1_1331r_LNP = 0.
 
double Clq1_1332i_LNP = 0.
 
double Clq1_1332r_LNP = 0.
 
double Clq1_1333i_LNP = 0.
 
double Clq1_1333r_LNP = 0.
 
double Clq1_2211r_LNP = 0.
 
double Clq1_2212i_LNP = 0.
 
double Clq1_2212r_LNP = 0.
 
double Clq1_2213i_LNP = 0.
 
double Clq1_2213r_LNP = 0.
 
double Clq1_2222r_LNP = 0.
 
double Clq1_2223i_LNP = 0.
 
double Clq1_2223r_LNP = 0.
 
double Clq1_2233r_LNP = 0.
 
double Clq1_2311i_LNP = 0.
 
double Clq1_2311r_LNP = 0.
 
double Clq1_2312i_LNP = 0.
 
double Clq1_2312r_LNP = 0.
 
double Clq1_2313i_LNP = 0.
 
double Clq1_2313r_LNP = 0.
 
double Clq1_2321i_LNP = 0.
 
double Clq1_2321r_LNP = 0.
 
double Clq1_2322i_LNP = 0.
 
double Clq1_2322r_LNP = 0.
 
double Clq1_2323i_LNP = 0.
 
double Clq1_2323r_LNP = 0.
 
double Clq1_2331i_LNP = 0.
 
double Clq1_2331r_LNP = 0.
 
double Clq1_2332i_LNP = 0.
 
double Clq1_2332r_LNP = 0.
 
double Clq1_2333i_LNP = 0.
 
double Clq1_2333r_LNP = 0.
 
double Clq1_3311r_LNP = 0.
 
double Clq1_3312i_LNP = 0.
 
double Clq1_3312r_LNP = 0.
 
double Clq1_3313i_LNP = 0.
 
double Clq1_3313r_LNP = 0.
 
double Clq1_3322r_LNP = 0.
 
double Clq1_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{lq}^{(1)})_{ijkm}\) (Imaginary part). More...
 
double Clq1_3323r_LNP = 0.
 
double Clq1_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{lq}^{(1)})_{ijkm}\) (Real part and pure real operator). More...
 
double Clq3_1111r_LNP = 0.
 
double Clq3_1112i_LNP = 0.
 
double Clq3_1112r_LNP = 0.
 
double Clq3_1113i_LNP = 0.
 
double Clq3_1113r_LNP = 0.
 
double Clq3_1122r_LNP = 0.
 
double Clq3_1123i_LNP = 0.
 
double Clq3_1123r_LNP = 0.
 
double Clq3_1133r_LNP = 0.
 
double Clq3_1211i_LNP = 0.
 
double Clq3_1211r_LNP = 0.
 
double Clq3_1212i_LNP = 0.
 
double Clq3_1212r_LNP = 0.
 
double Clq3_1213i_LNP = 0.
 
double Clq3_1213r_LNP = 0.
 
double Clq3_1221i_LNP = 0.
 
double Clq3_1221r_LNP = 0.
 
double Clq3_1222i_LNP = 0.
 
double Clq3_1222r_LNP = 0.
 
double Clq3_1223i_LNP = 0.
 
double Clq3_1223r_LNP = 0.
 
double Clq3_1231i_LNP = 0.
 
double Clq3_1231r_LNP = 0.
 
double Clq3_1232i_LNP = 0.
 
double Clq3_1232r_LNP = 0.
 
double Clq3_1233i_LNP = 0.
 
double Clq3_1233r_LNP = 0.
 
double Clq3_1311i_LNP = 0.
 
double Clq3_1311r_LNP = 0.
 
double Clq3_1312i_LNP = 0.
 
double Clq3_1312r_LNP = 0.
 
double Clq3_1313i_LNP = 0.
 
double Clq3_1313r_LNP = 0.
 
double Clq3_1321i_LNP = 0.
 
double Clq3_1321r_LNP = 0.
 
double Clq3_1322i_LNP = 0.
 
double Clq3_1322r_LNP = 0.
 
double Clq3_1323i_LNP = 0.
 
double Clq3_1323r_LNP = 0.
 
double Clq3_1331i_LNP = 0.
 
double Clq3_1331r_LNP = 0.
 
double Clq3_1332i_LNP = 0.
 
double Clq3_1332r_LNP = 0.
 
double Clq3_1333i_LNP = 0.
 
double Clq3_1333r_LNP = 0.
 
double Clq3_2211r_LNP = 0.
 
double Clq3_2212i_LNP = 0.
 
double Clq3_2212r_LNP = 0.
 
double Clq3_2213i_LNP = 0.
 
double Clq3_2213r_LNP = 0.
 
double Clq3_2222r_LNP = 0.
 
double Clq3_2223i_LNP = 0.
 
double Clq3_2223r_LNP = 0.
 
double Clq3_2233r_LNP = 0.
 
double Clq3_2311i_LNP = 0.
 
double Clq3_2311r_LNP = 0.
 
double Clq3_2312i_LNP = 0.
 
double Clq3_2312r_LNP = 0.
 
double Clq3_2313i_LNP = 0.
 
double Clq3_2313r_LNP = 0.
 
double Clq3_2321i_LNP = 0.
 
double Clq3_2321r_LNP = 0.
 
double Clq3_2322i_LNP = 0.
 
double Clq3_2322r_LNP = 0.
 
double Clq3_2323i_LNP = 0.
 
double Clq3_2323r_LNP = 0.
 
double Clq3_2331i_LNP = 0.
 
double Clq3_2331r_LNP = 0.
 
double Clq3_2332i_LNP = 0.
 
double Clq3_2332r_LNP = 0.
 
double Clq3_2333i_LNP = 0.
 
double Clq3_2333r_LNP = 0.
 
double Clq3_3311r_LNP = 0.
 
double Clq3_3312i_LNP = 0.
 
double Clq3_3312r_LNP = 0.
 
double Clq3_3313i_LNP = 0.
 
double Clq3_3313r_LNP = 0.
 
double Clq3_3322r_LNP = 0.
 
double Clq3_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{lq}^{(3)})_{ijkm}\) (Imaginary part). More...
 
double Clq3_3323r_LNP = 0.
 
double Clq3_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{lq}^{(3)})_{ijkm}\) (Real part and pure real operator). More...
 
double Clu_1111r_LNP = 0.
 
double Clu_1112i_LNP = 0.
 
double Clu_1112r_LNP = 0.
 
double Clu_1113i_LNP = 0.
 
double Clu_1113r_LNP = 0.
 
double Clu_1122r_LNP = 0.
 
double Clu_1123i_LNP = 0.
 
double Clu_1123r_LNP = 0.
 
double Clu_1133r_LNP = 0.
 
double Clu_1211i_LNP = 0.
 
double Clu_1211r_LNP = 0.
 
double Clu_1212i_LNP = 0.
 
double Clu_1212r_LNP = 0.
 
double Clu_1213i_LNP = 0.
 
double Clu_1213r_LNP = 0.
 
double Clu_1221i_LNP = 0.
 
double Clu_1221r_LNP = 0.
 
double Clu_1222i_LNP = 0.
 
double Clu_1222r_LNP = 0.
 
double Clu_1223i_LNP = 0.
 
double Clu_1223r_LNP = 0.
 
double Clu_1231i_LNP = 0.
 
double Clu_1231r_LNP = 0.
 
double Clu_1232i_LNP = 0.
 
double Clu_1232r_LNP = 0.
 
double Clu_1233i_LNP = 0.
 
double Clu_1233r_LNP = 0.
 
double Clu_1311i_LNP = 0.
 
double Clu_1311r_LNP = 0.
 
double Clu_1312i_LNP = 0.
 
double Clu_1312r_LNP = 0.
 
double Clu_1313i_LNP = 0.
 
double Clu_1313r_LNP = 0.
 
double Clu_1321i_LNP = 0.
 
double Clu_1321r_LNP = 0.
 
double Clu_1322i_LNP = 0.
 
double Clu_1322r_LNP = 0.
 
double Clu_1323i_LNP = 0.
 
double Clu_1323r_LNP = 0.
 
double Clu_1331i_LNP = 0.
 
double Clu_1331r_LNP = 0.
 
double Clu_1332i_LNP = 0.
 
double Clu_1332r_LNP = 0.
 
double Clu_1333i_LNP = 0.
 
double Clu_1333r_LNP = 0.
 
double Clu_2211r_LNP = 0.
 
double Clu_2212i_LNP = 0.
 
double Clu_2212r_LNP = 0.
 
double Clu_2213i_LNP = 0.
 
double Clu_2213r_LNP = 0.
 
double Clu_2222r_LNP = 0.
 
double Clu_2223i_LNP = 0.
 
double Clu_2223r_LNP = 0.
 
double Clu_2233r_LNP = 0.
 
double Clu_2311i_LNP = 0.
 
double Clu_2311r_LNP = 0.
 
double Clu_2312i_LNP = 0.
 
double Clu_2312r_LNP = 0.
 
double Clu_2313i_LNP = 0.
 
double Clu_2313r_LNP = 0.
 
double Clu_2321i_LNP = 0.
 
double Clu_2321r_LNP = 0.
 
double Clu_2322i_LNP = 0.
 
double Clu_2322r_LNP = 0.
 
double Clu_2323i_LNP = 0.
 
double Clu_2323r_LNP = 0.
 
double Clu_2331i_LNP = 0.
 
double Clu_2331r_LNP = 0.
 
double Clu_2332i_LNP = 0.
 
double Clu_2332r_LNP = 0.
 
double Clu_2333i_LNP = 0.
 
double Clu_2333r_LNP = 0.
 
double Clu_3311r_LNP = 0.
 
double Clu_3312i_LNP = 0.
 
double Clu_3312r_LNP = 0.
 
double Clu_3313i_LNP = 0.
 
double Clu_3313r_LNP = 0.
 
double Clu_3322r_LNP = 0.
 
double Clu_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{lu})_{ijkm}\) (Imaginary part). More...
 
double Clu_3323r_LNP = 0.
 
double Clu_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{lu})_{ijkm}\) (Real part and pure real operator). More...
 
double cNLOd6
 Parameter to control the inclusion of finite NLO corrections, when available. More...
 
double Cqd1_1111r_LNP = 0.
 
double Cqd1_1112i_LNP = 0.
 
double Cqd1_1112r_LNP = 0.
 
double Cqd1_1113i_LNP = 0.
 
double Cqd1_1113r_LNP = 0.
 
double Cqd1_1122r_LNP = 0.
 
double Cqd1_1123i_LNP = 0.
 
double Cqd1_1123r_LNP = 0.
 
double Cqd1_1133r_LNP = 0.
 
double Cqd1_1211i_LNP = 0.
 
double Cqd1_1211r_LNP = 0.
 
double Cqd1_1212i_LNP = 0.
 
double Cqd1_1212r_LNP = 0.
 
double Cqd1_1213i_LNP = 0.
 
double Cqd1_1213r_LNP = 0.
 
double Cqd1_1221i_LNP = 0.
 
double Cqd1_1221r_LNP = 0.
 
double Cqd1_1222i_LNP = 0.
 
double Cqd1_1222r_LNP = 0.
 
double Cqd1_1223i_LNP = 0.
 
double Cqd1_1223r_LNP = 0.
 
double Cqd1_1231i_LNP = 0.
 
double Cqd1_1231r_LNP = 0.
 
double Cqd1_1232i_LNP = 0.
 
double Cqd1_1232r_LNP = 0.
 
double Cqd1_1233i_LNP = 0.
 
double Cqd1_1233r_LNP = 0.
 
double Cqd1_1311i_LNP = 0.
 
double Cqd1_1311r_LNP = 0.
 
double Cqd1_1312i_LNP = 0.
 
double Cqd1_1312r_LNP = 0.
 
double Cqd1_1313i_LNP = 0.
 
double Cqd1_1313r_LNP = 0.
 
double Cqd1_1321i_LNP = 0.
 
double Cqd1_1321r_LNP = 0.
 
double Cqd1_1322i_LNP = 0.
 
double Cqd1_1322r_LNP = 0.
 
double Cqd1_1323i_LNP = 0.
 
double Cqd1_1323r_LNP = 0.
 
double Cqd1_1331i_LNP = 0.
 
double Cqd1_1331r_LNP = 0.
 
double Cqd1_1332i_LNP = 0.
 
double Cqd1_1332r_LNP = 0.
 
double Cqd1_1333i_LNP = 0.
 
double Cqd1_1333r_LNP = 0.
 
double Cqd1_2211r_LNP = 0.
 
double Cqd1_2212i_LNP = 0.
 
double Cqd1_2212r_LNP = 0.
 
double Cqd1_2213i_LNP = 0.
 
double Cqd1_2213r_LNP = 0.
 
double Cqd1_2222r_LNP = 0.
 
double Cqd1_2223i_LNP = 0.
 
double Cqd1_2223r_LNP = 0.
 
double Cqd1_2233r_LNP = 0.
 
double Cqd1_2311i_LNP = 0.
 
double Cqd1_2311r_LNP = 0.
 
double Cqd1_2312i_LNP = 0.
 
double Cqd1_2312r_LNP = 0.
 
double Cqd1_2313i_LNP = 0.
 
double Cqd1_2313r_LNP = 0.
 
double Cqd1_2321i_LNP = 0.
 
double Cqd1_2321r_LNP = 0.
 
double Cqd1_2322i_LNP = 0.
 
double Cqd1_2322r_LNP = 0.
 
double Cqd1_2323i_LNP = 0.
 
double Cqd1_2323r_LNP = 0.
 
double Cqd1_2331i_LNP = 0.
 
double Cqd1_2331r_LNP = 0.
 
double Cqd1_2332i_LNP = 0.
 
double Cqd1_2332r_LNP = 0.
 
double Cqd1_2333i_LNP = 0.
 
double Cqd1_2333r_LNP = 0.
 
double Cqd1_3311r_LNP = 0.
 
double Cqd1_3312i_LNP = 0.
 
double Cqd1_3312r_LNP = 0.
 
double Cqd1_3313i_LNP = 0.
 
double Cqd1_3313r_LNP = 0.
 
double Cqd1_3322r_LNP = 0.
 
double Cqd1_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{qd}^{(1)})_{ijkm}\) (Imaginary part). More...
 
double Cqd1_3323r_LNP = 0.
 
double Cqd1_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{qd}^{(1)})_{ijkm}\) (Real part and pure real operator). More...
 
double Cqd8_1111r_LNP = 0.
 
double Cqd8_1112i_LNP = 0.
 
double Cqd8_1112r_LNP = 0.
 
double Cqd8_1113i_LNP = 0.
 
double Cqd8_1113r_LNP = 0.
 
double Cqd8_1122r_LNP = 0.
 
double Cqd8_1123i_LNP = 0.
 
double Cqd8_1123r_LNP = 0.
 
double Cqd8_1133r_LNP = 0.
 
double Cqd8_1211i_LNP = 0.
 
double Cqd8_1211r_LNP = 0.
 
double Cqd8_1212i_LNP = 0.
 
double Cqd8_1212r_LNP = 0.
 
double Cqd8_1213i_LNP = 0.
 
double Cqd8_1213r_LNP = 0.
 
double Cqd8_1221i_LNP = 0.
 
double Cqd8_1221r_LNP = 0.
 
double Cqd8_1222i_LNP = 0.
 
double Cqd8_1222r_LNP = 0.
 
double Cqd8_1223i_LNP = 0.
 
double Cqd8_1223r_LNP = 0.
 
double Cqd8_1231i_LNP = 0.
 
double Cqd8_1231r_LNP = 0.
 
double Cqd8_1232i_LNP = 0.
 
double Cqd8_1232r_LNP = 0.
 
double Cqd8_1233i_LNP = 0.
 
double Cqd8_1233r_LNP = 0.
 
double Cqd8_1311i_LNP = 0.
 
double Cqd8_1311r_LNP = 0.
 
double Cqd8_1312i_LNP = 0.
 
double Cqd8_1312r_LNP = 0.
 
double Cqd8_1313i_LNP = 0.
 
double Cqd8_1313r_LNP = 0.
 
double Cqd8_1321i_LNP = 0.
 
double Cqd8_1321r_LNP = 0.
 
double Cqd8_1322i_LNP = 0.
 
double Cqd8_1322r_LNP = 0.
 
double Cqd8_1323i_LNP = 0.
 
double Cqd8_1323r_LNP = 0.
 
double Cqd8_1331i_LNP = 0.
 
double Cqd8_1331r_LNP = 0.
 
double Cqd8_1332i_LNP = 0.
 
double Cqd8_1332r_LNP = 0.
 
double Cqd8_1333i_LNP = 0.
 
double Cqd8_1333r_LNP = 0.
 
double Cqd8_2211r_LNP = 0.
 
double Cqd8_2212i_LNP = 0.
 
double Cqd8_2212r_LNP = 0.
 
double Cqd8_2213i_LNP = 0.
 
double Cqd8_2213r_LNP = 0.
 
double Cqd8_2222r_LNP = 0.
 
double Cqd8_2223i_LNP = 0.
 
double Cqd8_2223r_LNP = 0.
 
double Cqd8_2233r_LNP = 0.
 
double Cqd8_2311i_LNP = 0.
 
double Cqd8_2311r_LNP = 0.
 
double Cqd8_2312i_LNP = 0.
 
double Cqd8_2312r_LNP = 0.
 
double Cqd8_2313i_LNP = 0.
 
double Cqd8_2313r_LNP = 0.
 
double Cqd8_2321i_LNP = 0.
 
double Cqd8_2321r_LNP = 0.
 
double Cqd8_2322i_LNP = 0.
 
double Cqd8_2322r_LNP = 0.
 
double Cqd8_2323i_LNP = 0.
 
double Cqd8_2323r_LNP = 0.
 
double Cqd8_2331i_LNP = 0.
 
double Cqd8_2331r_LNP = 0.
 
double Cqd8_2332i_LNP = 0.
 
double Cqd8_2332r_LNP = 0.
 
double Cqd8_2333i_LNP = 0.
 
double Cqd8_2333r_LNP = 0.
 
double Cqd8_3311r_LNP = 0.
 
double Cqd8_3312i_LNP = 0.
 
double Cqd8_3312r_LNP = 0.
 
double Cqd8_3313i_LNP = 0.
 
double Cqd8_3313r_LNP = 0.
 
double Cqd8_3322r_LNP = 0.
 
double Cqd8_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{qd}^{(8)})_{ijkm}\) (Imaginary part). More...
 
double Cqd8_3323r_LNP = 0.
 
double Cqd8_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{qd}^{(8)})_{ijkm}\) (Real part and pure real operator). More...
 
double Cqe_1111r_LNP = 0.
 
double Cqe_1112i_LNP = 0.
 
double Cqe_1112r_LNP = 0.
 
double Cqe_1113i_LNP = 0.
 
double Cqe_1113r_LNP = 0.
 
double Cqe_1122r_LNP = 0.
 
double Cqe_1123i_LNP = 0.
 
double Cqe_1123r_LNP = 0.
 
double Cqe_1133r_LNP = 0.
 
double Cqe_1211i_LNP = 0.
 
double Cqe_1211r_LNP = 0.
 
double Cqe_1212i_LNP = 0.
 
double Cqe_1212r_LNP = 0.
 
double Cqe_1213i_LNP = 0.
 
double Cqe_1213r_LNP = 0.
 
double Cqe_1221i_LNP = 0.
 
double Cqe_1221r_LNP = 0.
 
double Cqe_1222i_LNP = 0.
 
double Cqe_1222r_LNP = 0.
 
double Cqe_1223i_LNP = 0.
 
double Cqe_1223r_LNP = 0.
 
double Cqe_1231i_LNP = 0.
 
double Cqe_1231r_LNP = 0.
 
double Cqe_1232i_LNP = 0.
 
double Cqe_1232r_LNP = 0.
 
double Cqe_1233i_LNP = 0.
 
double Cqe_1233r_LNP = 0.
 
double Cqe_1311i_LNP = 0.
 
double Cqe_1311r_LNP = 0.
 
double Cqe_1312i_LNP = 0.
 
double Cqe_1312r_LNP = 0.
 
double Cqe_1313i_LNP = 0.
 
double Cqe_1313r_LNP = 0.
 
double Cqe_1321i_LNP = 0.
 
double Cqe_1321r_LNP = 0.
 
double Cqe_1322i_LNP = 0.
 
double Cqe_1322r_LNP = 0.
 
double Cqe_1323i_LNP = 0.
 
double Cqe_1323r_LNP = 0.
 
double Cqe_1331i_LNP = 0.
 
double Cqe_1331r_LNP = 0.
 
double Cqe_1332i_LNP = 0.
 
double Cqe_1332r_LNP = 0.
 
double Cqe_1333i_LNP = 0.
 
double Cqe_1333r_LNP = 0.
 
double Cqe_2211r_LNP = 0.
 
double Cqe_2212i_LNP = 0.
 
double Cqe_2212r_LNP = 0.
 
double Cqe_2213i_LNP = 0.
 
double Cqe_2213r_LNP = 0.
 
double Cqe_2222r_LNP = 0.
 
double Cqe_2223i_LNP = 0.
 
double Cqe_2223r_LNP = 0.
 
double Cqe_2233r_LNP = 0.
 
double Cqe_2311i_LNP = 0.
 
double Cqe_2311r_LNP = 0.
 
double Cqe_2312i_LNP = 0.
 
double Cqe_2312r_LNP = 0.
 
double Cqe_2313i_LNP = 0.
 
double Cqe_2313r_LNP = 0.
 
double Cqe_2321i_LNP = 0.
 
double Cqe_2321r_LNP = 0.
 
double Cqe_2322i_LNP = 0.
 
double Cqe_2322r_LNP = 0.
 
double Cqe_2323i_LNP = 0.
 
double Cqe_2323r_LNP = 0.
 
double Cqe_2331i_LNP = 0.
 
double Cqe_2331r_LNP = 0.
 
double Cqe_2332i_LNP = 0.
 
double Cqe_2332r_LNP = 0.
 
double Cqe_2333i_LNP = 0.
 
double Cqe_2333r_LNP = 0.
 
double Cqe_3311r_LNP = 0.
 
double Cqe_3312i_LNP = 0.
 
double Cqe_3312r_LNP = 0.
 
double Cqe_3313i_LNP = 0.
 
double Cqe_3313r_LNP = 0.
 
double Cqe_3322r_LNP = 0.
 
double Cqe_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{qe})_{ijkm}\) (Imaginary part). More...
 
double Cqe_3323r_LNP = 0.
 
double Cqe_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{qe})_{ijkm}\) (Real part and pure real operator). More...
 
double Cqq1_1111r_LNP = 0.
 
double Cqq1_1112i_LNP = 0.
 
double Cqq1_1112r_LNP = 0.
 
double Cqq1_1113i_LNP = 0.
 
double Cqq1_1113r_LNP = 0.
 
double Cqq1_1122r_LNP = 0.
 
double Cqq1_1123i_LNP = 0.
 
double Cqq1_1123r_LNP = 0.
 
double Cqq1_1133r_LNP = 0.
 
double Cqq1_1212i_LNP = 0.
 
double Cqq1_1212r_LNP = 0.
 
double Cqq1_1213i_LNP = 0.
 
double Cqq1_1213r_LNP = 0.
 
double Cqq1_1221r_LNP = 0.
 
double Cqq1_1222i_LNP = 0.
 
double Cqq1_1222r_LNP = 0.
 
double Cqq1_1223i_LNP = 0.
 
double Cqq1_1223r_LNP = 0.
 
double Cqq1_1231i_LNP = 0.
 
double Cqq1_1231r_LNP = 0.
 
double Cqq1_1232i_LNP = 0.
 
double Cqq1_1232r_LNP = 0.
 
double Cqq1_1233i_LNP = 0.
 
double Cqq1_1233r_LNP = 0.
 
double Cqq1_1313i_LNP = 0.
 
double Cqq1_1313r_LNP = 0.
 
double Cqq1_1322i_LNP = 0.
 
double Cqq1_1322r_LNP = 0.
 
double Cqq1_1323i_LNP = 0.
 
double Cqq1_1323r_LNP = 0.
 
double Cqq1_1331r_LNP = 0.
 
double Cqq1_1332i_LNP = 0.
 
double Cqq1_1332r_LNP = 0.
 
double Cqq1_1333i_LNP = 0.
 
double Cqq1_1333r_LNP = 0.
 
double Cqq1_2222r_LNP = 0.
 
double Cqq1_2223i_LNP = 0.
 
double Cqq1_2223r_LNP = 0.
 
double Cqq1_2233r_LNP = 0.
 
double Cqq1_2323i_LNP = 0.
 
double Cqq1_2323r_LNP = 0.
 
double Cqq1_2332r_LNP = 0.
 
double Cqq1_2333i_LNP = 0.
 The dimension-6 operator coefficient \((C_{qq}^{(1)})_{ijkm}\) (Imaginary part). More...
 
double Cqq1_2333r_LNP = 0.
 
double Cqq1_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{qq}^{(1)})_{ijkm}\) (Real part and pure real operator). More...
 
double Cqq3_1111r_LNP = 0.
 
double Cqq3_1112i_LNP = 0.
 
double Cqq3_1112r_LNP = 0.
 
double Cqq3_1113i_LNP = 0.
 
double Cqq3_1113r_LNP = 0.
 
double Cqq3_1122r_LNP = 0.
 
double Cqq3_1123i_LNP = 0.
 
double Cqq3_1123r_LNP = 0.
 
double Cqq3_1133r_LNP = 0.
 
double Cqq3_1212i_LNP = 0.
 
double Cqq3_1212r_LNP = 0.
 
double Cqq3_1213i_LNP = 0.
 
double Cqq3_1213r_LNP = 0.
 
double Cqq3_1221r_LNP = 0.
 
double Cqq3_1222i_LNP = 0.
 
double Cqq3_1222r_LNP = 0.
 
double Cqq3_1223i_LNP = 0.
 
double Cqq3_1223r_LNP = 0.
 
double Cqq3_1231i_LNP = 0.
 
double Cqq3_1231r_LNP = 0.
 
double Cqq3_1232i_LNP = 0.
 
double Cqq3_1232r_LNP = 0.
 
double Cqq3_1233i_LNP = 0.
 
double Cqq3_1233r_LNP = 0.
 
double Cqq3_1313i_LNP = 0.
 
double Cqq3_1313r_LNP = 0.
 
double Cqq3_1322i_LNP = 0.
 
double Cqq3_1322r_LNP = 0.
 
double Cqq3_1323i_LNP = 0.
 
double Cqq3_1323r_LNP = 0.
 
double Cqq3_1331r_LNP = 0.
 
double Cqq3_1332i_LNP = 0.
 
double Cqq3_1332r_LNP = 0.
 
double Cqq3_1333i_LNP = 0.
 
double Cqq3_1333r_LNP = 0.
 
double Cqq3_2222r_LNP = 0.
 
double Cqq3_2223i_LNP = 0.
 
double Cqq3_2223r_LNP = 0.
 
double Cqq3_2233r_LNP = 0.
 
double Cqq3_2323i_LNP = 0.
 
double Cqq3_2323r_LNP = 0.
 
double Cqq3_2332r_LNP = 0.
 
double Cqq3_2333i_LNP = 0.
 The dimension-6 operator coefficient \((C_{qq}^{(3)})_{ijkm}\) (Imaginary part). More...
 
double Cqq3_2333r_LNP = 0.
 
double Cqq3_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{qq}^{(3)})_{ijkm}\) (Real part and pure real operator). More...
 
double Cqu1_1111r_LNP = 0.
 
double Cqu1_1112i_LNP = 0.
 
double Cqu1_1112r_LNP = 0.
 
double Cqu1_1113i_LNP = 0.
 
double Cqu1_1113r_LNP = 0.
 
double Cqu1_1122r_LNP = 0.
 
double Cqu1_1123i_LNP = 0.
 
double Cqu1_1123r_LNP = 0.
 
double Cqu1_1133r_LNP = 0.
 
double Cqu1_1211i_LNP = 0.
 
double Cqu1_1211r_LNP = 0.
 
double Cqu1_1212i_LNP = 0.
 
double Cqu1_1212r_LNP = 0.
 
double Cqu1_1213i_LNP = 0.
 
double Cqu1_1213r_LNP = 0.
 
double Cqu1_1221i_LNP = 0.
 
double Cqu1_1221r_LNP = 0.
 
double Cqu1_1222i_LNP = 0.
 
double Cqu1_1222r_LNP = 0.
 
double Cqu1_1223i_LNP = 0.
 
double Cqu1_1223r_LNP = 0.
 
double Cqu1_1231i_LNP = 0.
 
double Cqu1_1231r_LNP = 0.
 
double Cqu1_1232i_LNP = 0.
 
double Cqu1_1232r_LNP = 0.
 
double Cqu1_1233i_LNP = 0.
 
double Cqu1_1233r_LNP = 0.
 
double Cqu1_1311i_LNP = 0.
 
double Cqu1_1311r_LNP = 0.
 
double Cqu1_1312i_LNP = 0.
 
double Cqu1_1312r_LNP = 0.
 
double Cqu1_1313i_LNP = 0.
 
double Cqu1_1313r_LNP = 0.
 
double Cqu1_1321i_LNP = 0.
 
double Cqu1_1321r_LNP = 0.
 
double Cqu1_1322i_LNP = 0.
 
double Cqu1_1322r_LNP = 0.
 
double Cqu1_1323i_LNP = 0.
 
double Cqu1_1323r_LNP = 0.
 
double Cqu1_1331i_LNP = 0.
 
double Cqu1_1331r_LNP = 0.
 
double Cqu1_1332i_LNP = 0.
 
double Cqu1_1332r_LNP = 0.
 
double Cqu1_1333i_LNP = 0.
 
double Cqu1_1333r_LNP = 0.
 
double Cqu1_2211r_LNP = 0.
 
double Cqu1_2212i_LNP = 0.
 
double Cqu1_2212r_LNP = 0.
 
double Cqu1_2213i_LNP = 0.
 
double Cqu1_2213r_LNP = 0.
 
double Cqu1_2222r_LNP = 0.
 
double Cqu1_2223i_LNP = 0.
 
double Cqu1_2223r_LNP = 0.
 
double Cqu1_2233r_LNP = 0.
 
double Cqu1_2311i_LNP = 0.
 
double Cqu1_2311r_LNP = 0.
 
double Cqu1_2312i_LNP = 0.
 
double Cqu1_2312r_LNP = 0.
 
double Cqu1_2313i_LNP = 0.
 
double Cqu1_2313r_LNP = 0.
 
double Cqu1_2321i_LNP = 0.
 
double Cqu1_2321r_LNP = 0.
 
double Cqu1_2322i_LNP = 0.
 
double Cqu1_2322r_LNP = 0.
 
double Cqu1_2323i_LNP = 0.
 
double Cqu1_2323r_LNP = 0.
 
double Cqu1_2331i_LNP = 0.
 
double Cqu1_2331r_LNP = 0.
 
double Cqu1_2332i_LNP = 0.
 
double Cqu1_2332r_LNP = 0.
 
double Cqu1_2333i_LNP = 0.
 
double Cqu1_2333r_LNP = 0.
 
double Cqu1_3311r_LNP = 0.
 
double Cqu1_3312i_LNP = 0.
 
double Cqu1_3312r_LNP = 0.
 
double Cqu1_3313i_LNP = 0.
 
double Cqu1_3313r_LNP = 0.
 
double Cqu1_3322r_LNP = 0.
 
double Cqu1_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{qu}^{(1)})_{ijkm}\) (Imaginary part). More...
 
double Cqu1_3323r_LNP = 0.
 
double Cqu1_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{qu}^{(1)})_{ijkm}\) (Real part and pure real operator). More...
 
double Cqu8_1111r_LNP = 0.
 
double Cqu8_1112i_LNP = 0.
 
double Cqu8_1112r_LNP = 0.
 
double Cqu8_1113i_LNP = 0.
 
double Cqu8_1113r_LNP = 0.
 
double Cqu8_1122r_LNP = 0.
 
double Cqu8_1123i_LNP = 0.
 
double Cqu8_1123r_LNP = 0.
 
double Cqu8_1133r_LNP = 0.
 
double Cqu8_1211i_LNP = 0.
 
double Cqu8_1211r_LNP = 0.
 
double Cqu8_1212i_LNP = 0.
 
double Cqu8_1212r_LNP = 0.
 
double Cqu8_1213i_LNP = 0.
 
double Cqu8_1213r_LNP = 0.
 
double Cqu8_1221i_LNP = 0.
 
double Cqu8_1221r_LNP = 0.
 
double Cqu8_1222i_LNP = 0.
 
double Cqu8_1222r_LNP = 0.
 
double Cqu8_1223i_LNP = 0.
 
double Cqu8_1223r_LNP = 0.
 
double Cqu8_1231i_LNP = 0.
 
double Cqu8_1231r_LNP = 0.
 
double Cqu8_1232i_LNP = 0.
 
double Cqu8_1232r_LNP = 0.
 
double Cqu8_1233i_LNP = 0.
 
double Cqu8_1233r_LNP = 0.
 
double Cqu8_1311i_LNP = 0.
 
double Cqu8_1311r_LNP = 0.
 
double Cqu8_1312i_LNP = 0.
 
double Cqu8_1312r_LNP = 0.
 
double Cqu8_1313i_LNP = 0.
 
double Cqu8_1313r_LNP = 0.
 
double Cqu8_1321i_LNP = 0.
 
double Cqu8_1321r_LNP = 0.
 
double Cqu8_1322i_LNP = 0.
 
double Cqu8_1322r_LNP = 0.
 
double Cqu8_1323i_LNP = 0.
 
double Cqu8_1323r_LNP = 0.
 
double Cqu8_1331i_LNP = 0.
 
double Cqu8_1331r_LNP = 0.
 
double Cqu8_1332i_LNP = 0.
 
double Cqu8_1332r_LNP = 0.
 
double Cqu8_1333i_LNP = 0.
 
double Cqu8_1333r_LNP = 0.
 
double Cqu8_2211r_LNP = 0.
 
double Cqu8_2212i_LNP = 0.
 
double Cqu8_2212r_LNP = 0.
 
double Cqu8_2213i_LNP = 0.
 
double Cqu8_2213r_LNP = 0.
 
double Cqu8_2222r_LNP = 0.
 
double Cqu8_2223i_LNP = 0.
 
double Cqu8_2223r_LNP = 0.
 
double Cqu8_2233r_LNP = 0.
 
double Cqu8_2311i_LNP = 0.
 
double Cqu8_2311r_LNP = 0.
 
double Cqu8_2312i_LNP = 0.
 
double Cqu8_2312r_LNP = 0.
 
double Cqu8_2313i_LNP = 0.
 
double Cqu8_2313r_LNP = 0.
 
double Cqu8_2321i_LNP = 0.
 
double Cqu8_2321r_LNP = 0.
 
double Cqu8_2322i_LNP = 0.
 
double Cqu8_2322r_LNP = 0.
 
double Cqu8_2323i_LNP = 0.
 
double Cqu8_2323r_LNP = 0.
 
double Cqu8_2331i_LNP = 0.
 
double Cqu8_2331r_LNP = 0.
 
double Cqu8_2332i_LNP = 0.
 
double Cqu8_2332r_LNP = 0.
 
double Cqu8_2333i_LNP = 0.
 
double Cqu8_2333r_LNP = 0.
 
double Cqu8_3311r_LNP = 0.
 
double Cqu8_3312i_LNP = 0.
 
double Cqu8_3312r_LNP = 0.
 
double Cqu8_3313i_LNP = 0.
 
double Cqu8_3313r_LNP = 0.
 
double Cqu8_3322r_LNP = 0.
 
double Cqu8_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{qu}^{(8)})_{ijkm}\) (Imaginary part). More...
 
double Cqu8_3323r_LNP = 0.
 
double Cqu8_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{qu}^{(8)})_{ijkm}\) (Real part and pure real operator). More...
 
double Cquqd1_1111i_LNP = 0.
 
double Cquqd1_1111r_LNP = 0.
 
double Cquqd1_1112i_LNP = 0.
 
double Cquqd1_1112r_LNP = 0.
 
double Cquqd1_1113i_LNP = 0.
 
double Cquqd1_1113r_LNP = 0.
 
double Cquqd1_1121i_LNP = 0.
 
double Cquqd1_1121r_LNP = 0.
 
double Cquqd1_1122i_LNP = 0.
 
double Cquqd1_1122r_LNP = 0.
 
double Cquqd1_1123i_LNP = 0.
 
double Cquqd1_1123r_LNP = 0.
 
double Cquqd1_1131i_LNP = 0.
 
double Cquqd1_1131r_LNP = 0.
 
double Cquqd1_1132i_LNP = 0.
 
double Cquqd1_1132r_LNP = 0.
 
double Cquqd1_1133i_LNP = 0.
 
double Cquqd1_1133r_LNP = 0.
 
double Cquqd1_1211i_LNP = 0.
 
double Cquqd1_1211r_LNP = 0.
 
double Cquqd1_1212i_LNP = 0.
 
double Cquqd1_1212r_LNP = 0.
 
double Cquqd1_1213i_LNP = 0.
 
double Cquqd1_1213r_LNP = 0.
 
double Cquqd1_1221i_LNP = 0.
 
double Cquqd1_1221r_LNP = 0.
 
double Cquqd1_1222i_LNP = 0.
 
double Cquqd1_1222r_LNP = 0.
 
double Cquqd1_1223i_LNP = 0.
 
double Cquqd1_1223r_LNP = 0.
 
double Cquqd1_1231i_LNP = 0.
 
double Cquqd1_1231r_LNP = 0.
 
double Cquqd1_1232i_LNP = 0.
 
double Cquqd1_1232r_LNP = 0.
 
double Cquqd1_1233i_LNP = 0.
 
double Cquqd1_1233r_LNP = 0.
 
double Cquqd1_1311i_LNP = 0.
 
double Cquqd1_1311r_LNP = 0.
 
double Cquqd1_1312i_LNP = 0.
 
double Cquqd1_1312r_LNP = 0.
 
double Cquqd1_1313i_LNP = 0.
 
double Cquqd1_1313r_LNP = 0.
 
double Cquqd1_1321i_LNP = 0.
 
double Cquqd1_1321r_LNP = 0.
 
double Cquqd1_1322i_LNP = 0.
 
double Cquqd1_1322r_LNP = 0.
 
double Cquqd1_1323i_LNP = 0.
 
double Cquqd1_1323r_LNP = 0.
 
double Cquqd1_1331i_LNP = 0.
 
double Cquqd1_1331r_LNP = 0.
 
double Cquqd1_1332i_LNP = 0.
 
double Cquqd1_1332r_LNP = 0.
 
double Cquqd1_1333i_LNP = 0.
 
double Cquqd1_1333r_LNP = 0.
 
double Cquqd1_2111i_LNP = 0.
 
double Cquqd1_2111r_LNP = 0.
 
double Cquqd1_2112i_LNP = 0.
 
double Cquqd1_2112r_LNP = 0.
 
double Cquqd1_2113i_LNP = 0.
 
double Cquqd1_2113r_LNP = 0.
 
double Cquqd1_2121i_LNP = 0.
 
double Cquqd1_2121r_LNP = 0.
 
double Cquqd1_2122i_LNP = 0.
 
double Cquqd1_2122r_LNP = 0.
 
double Cquqd1_2123i_LNP = 0.
 
double Cquqd1_2123r_LNP = 0.
 
double Cquqd1_2131i_LNP = 0.
 
double Cquqd1_2131r_LNP = 0.
 
double Cquqd1_2132i_LNP = 0.
 
double Cquqd1_2132r_LNP = 0.
 
double Cquqd1_2133i_LNP = 0.
 
double Cquqd1_2133r_LNP = 0.
 
double Cquqd1_2211i_LNP = 0.
 
double Cquqd1_2211r_LNP = 0.
 
double Cquqd1_2212i_LNP = 0.
 
double Cquqd1_2212r_LNP = 0.
 
double Cquqd1_2213i_LNP = 0.
 
double Cquqd1_2213r_LNP = 0.
 
double Cquqd1_2221i_LNP = 0.
 
double Cquqd1_2221r_LNP = 0.
 
double Cquqd1_2222i_LNP = 0.
 
double Cquqd1_2222r_LNP = 0.
 
double Cquqd1_2223i_LNP = 0.
 
double Cquqd1_2223r_LNP = 0.
 
double Cquqd1_2231i_LNP = 0.
 
double Cquqd1_2231r_LNP = 0.
 
double Cquqd1_2232i_LNP = 0.
 
double Cquqd1_2232r_LNP = 0.
 
double Cquqd1_2233i_LNP = 0.
 
double Cquqd1_2233r_LNP = 0.
 
double Cquqd1_2311i_LNP = 0.
 
double Cquqd1_2311r_LNP = 0.
 
double Cquqd1_2312i_LNP = 0.
 
double Cquqd1_2312r_LNP = 0.
 
double Cquqd1_2313i_LNP = 0.
 
double Cquqd1_2313r_LNP = 0.
 
double Cquqd1_2321i_LNP = 0.
 
double Cquqd1_2321r_LNP = 0.
 
double Cquqd1_2322i_LNP = 0.
 
double Cquqd1_2322r_LNP = 0.
 
double Cquqd1_2323i_LNP = 0.
 
double Cquqd1_2323r_LNP = 0.
 
double Cquqd1_2331i_LNP = 0.
 
double Cquqd1_2331r_LNP = 0.
 
double Cquqd1_2332i_LNP = 0.
 
double Cquqd1_2332r_LNP = 0.
 
double Cquqd1_2333i_LNP = 0.
 
double Cquqd1_2333r_LNP = 0.
 
double Cquqd1_3111i_LNP = 0.
 
double Cquqd1_3111r_LNP = 0.
 
double Cquqd1_3112i_LNP = 0.
 
double Cquqd1_3112r_LNP = 0.
 
double Cquqd1_3113i_LNP = 0.
 
double Cquqd1_3113r_LNP = 0.
 
double Cquqd1_3121i_LNP = 0.
 
double Cquqd1_3121r_LNP = 0.
 
double Cquqd1_3122i_LNP = 0.
 
double Cquqd1_3122r_LNP = 0.
 
double Cquqd1_3123i_LNP = 0.
 
double Cquqd1_3123r_LNP = 0.
 
double Cquqd1_3131i_LNP = 0.
 
double Cquqd1_3131r_LNP = 0.
 
double Cquqd1_3132i_LNP = 0.
 
double Cquqd1_3132r_LNP = 0.
 
double Cquqd1_3133i_LNP = 0.
 
double Cquqd1_3133r_LNP = 0.
 
double Cquqd1_3211i_LNP = 0.
 
double Cquqd1_3211r_LNP = 0.
 
double Cquqd1_3212i_LNP = 0.
 
double Cquqd1_3212r_LNP = 0.
 
double Cquqd1_3213i_LNP = 0.
 
double Cquqd1_3213r_LNP = 0.
 
double Cquqd1_3221i_LNP = 0.
 
double Cquqd1_3221r_LNP = 0.
 
double Cquqd1_3222i_LNP = 0.
 
double Cquqd1_3222r_LNP = 0.
 
double Cquqd1_3223i_LNP = 0.
 
double Cquqd1_3223r_LNP = 0.
 
double Cquqd1_3231i_LNP = 0.
 
double Cquqd1_3231r_LNP = 0.
 
double Cquqd1_3232i_LNP = 0.
 
double Cquqd1_3232r_LNP = 0.
 
double Cquqd1_3233i_LNP = 0.
 
double Cquqd1_3233r_LNP = 0.
 
double Cquqd1_3311i_LNP = 0.
 
double Cquqd1_3311r_LNP = 0.
 
double Cquqd1_3312i_LNP = 0.
 
double Cquqd1_3312r_LNP = 0.
 
double Cquqd1_3313i_LNP = 0.
 
double Cquqd1_3313r_LNP = 0.
 
double Cquqd1_3321i_LNP = 0.
 
double Cquqd1_3321r_LNP = 0.
 
double Cquqd1_3322i_LNP = 0.
 
double Cquqd1_3322r_LNP = 0.
 
double Cquqd1_3323i_LNP = 0.
 
double Cquqd1_3323r_LNP = 0.
 
double Cquqd1_3331i_LNP = 0.
 
double Cquqd1_3331r_LNP = 0.
 
double Cquqd1_3332i_LNP = 0.
 
double Cquqd1_3332r_LNP = 0.
 
double Cquqd1_3333i_LNP = 0.
 The dimension-6 operator coefficient \((C_{quqd}^{(1)})_{ijkm}\) (Imaginary part). More...
 
double Cquqd1_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{quqd}^{(1)})_{ijkm}\) (Real part and pure real operator). More...
 
double Cquqd8_1111i_LNP = 0.
 
double Cquqd8_1111r_LNP = 0.
 
double Cquqd8_1112i_LNP = 0.
 
double Cquqd8_1112r_LNP = 0.
 
double Cquqd8_1113i_LNP = 0.
 
double Cquqd8_1113r_LNP = 0.
 
double Cquqd8_1121i_LNP = 0.
 
double Cquqd8_1121r_LNP = 0.
 
double Cquqd8_1122i_LNP = 0.
 
double Cquqd8_1122r_LNP = 0.
 
double Cquqd8_1123i_LNP = 0.
 
double Cquqd8_1123r_LNP = 0.
 
double Cquqd8_1131i_LNP = 0.
 
double Cquqd8_1131r_LNP = 0.
 
double Cquqd8_1132i_LNP = 0.
 
double Cquqd8_1132r_LNP = 0.
 
double Cquqd8_1133i_LNP = 0.
 
double Cquqd8_1133r_LNP = 0.
 
double Cquqd8_1211i_LNP = 0.
 
double Cquqd8_1211r_LNP = 0.
 
double Cquqd8_1212i_LNP = 0.
 
double Cquqd8_1212r_LNP = 0.
 
double Cquqd8_1213i_LNP = 0.
 
double Cquqd8_1213r_LNP = 0.
 
double Cquqd8_1221i_LNP = 0.
 
double Cquqd8_1221r_LNP = 0.
 
double Cquqd8_1222i_LNP = 0.
 
double Cquqd8_1222r_LNP = 0.
 
double Cquqd8_1223i_LNP = 0.
 
double Cquqd8_1223r_LNP = 0.
 
double Cquqd8_1231i_LNP = 0.
 
double Cquqd8_1231r_LNP = 0.
 
double Cquqd8_1232i_LNP = 0.
 
double Cquqd8_1232r_LNP = 0.
 
double Cquqd8_1233i_LNP = 0.
 
double Cquqd8_1233r_LNP = 0.
 
double Cquqd8_1311i_LNP = 0.
 
double Cquqd8_1311r_LNP = 0.
 
double Cquqd8_1312i_LNP = 0.
 
double Cquqd8_1312r_LNP = 0.
 
double Cquqd8_1313i_LNP = 0.
 
double Cquqd8_1313r_LNP = 0.
 
double Cquqd8_1321i_LNP = 0.
 
double Cquqd8_1321r_LNP = 0.
 
double Cquqd8_1322i_LNP = 0.
 
double Cquqd8_1322r_LNP = 0.
 
double Cquqd8_1323i_LNP = 0.
 
double Cquqd8_1323r_LNP = 0.
 
double Cquqd8_1331i_LNP = 0.
 
double Cquqd8_1331r_LNP = 0.
 
double Cquqd8_1332i_LNP = 0.
 
double Cquqd8_1332r_LNP = 0.
 
double Cquqd8_1333i_LNP = 0.
 
double Cquqd8_1333r_LNP = 0.
 
double Cquqd8_2111i_LNP = 0.
 
double Cquqd8_2111r_LNP = 0.
 
double Cquqd8_2112i_LNP = 0.
 
double Cquqd8_2112r_LNP = 0.
 
double Cquqd8_2113i_LNP = 0.
 
double Cquqd8_2113r_LNP = 0.
 
double Cquqd8_2121i_LNP = 0.
 
double Cquqd8_2121r_LNP = 0.
 
double Cquqd8_2122i_LNP = 0.
 
double Cquqd8_2122r_LNP = 0.
 
double Cquqd8_2123i_LNP = 0.
 
double Cquqd8_2123r_LNP = 0.
 
double Cquqd8_2131i_LNP = 0.
 
double Cquqd8_2131r_LNP = 0.
 
double Cquqd8_2132i_LNP = 0.
 
double Cquqd8_2132r_LNP = 0.
 
double Cquqd8_2133i_LNP = 0.
 
double Cquqd8_2133r_LNP = 0.
 
double Cquqd8_2211i_LNP = 0.
 
double Cquqd8_2211r_LNP = 0.
 
double Cquqd8_2212i_LNP = 0.
 
double Cquqd8_2212r_LNP = 0.
 
double Cquqd8_2213i_LNP = 0.
 
double Cquqd8_2213r_LNP = 0.
 
double Cquqd8_2221i_LNP = 0.
 
double Cquqd8_2221r_LNP = 0.
 
double Cquqd8_2222i_LNP = 0.
 
double Cquqd8_2222r_LNP = 0.
 
double Cquqd8_2223i_LNP = 0.
 
double Cquqd8_2223r_LNP = 0.
 
double Cquqd8_2231i_LNP = 0.
 
double Cquqd8_2231r_LNP = 0.
 
double Cquqd8_2232i_LNP = 0.
 
double Cquqd8_2232r_LNP = 0.
 
double Cquqd8_2233i_LNP = 0.
 
double Cquqd8_2233r_LNP = 0.
 
double Cquqd8_2311i_LNP = 0.
 
double Cquqd8_2311r_LNP = 0.
 
double Cquqd8_2312i_LNP = 0.
 
double Cquqd8_2312r_LNP = 0.
 
double Cquqd8_2313i_LNP = 0.
 
double Cquqd8_2313r_LNP = 0.
 
double Cquqd8_2321i_LNP = 0.
 
double Cquqd8_2321r_LNP = 0.
 
double Cquqd8_2322i_LNP = 0.
 
double Cquqd8_2322r_LNP = 0.
 
double Cquqd8_2323i_LNP = 0.
 
double Cquqd8_2323r_LNP = 0.
 
double Cquqd8_2331i_LNP = 0.
 
double Cquqd8_2331r_LNP = 0.
 
double Cquqd8_2332i_LNP = 0.
 
double Cquqd8_2332r_LNP = 0.
 
double Cquqd8_2333i_LNP = 0.
 
double Cquqd8_2333r_LNP = 0.
 
double Cquqd8_3111i_LNP = 0.
 
double Cquqd8_3111r_LNP = 0.
 
double Cquqd8_3112i_LNP = 0.
 
double Cquqd8_3112r_LNP = 0.
 
double Cquqd8_3113i_LNP = 0.
 
double Cquqd8_3113r_LNP = 0.
 
double Cquqd8_3121i_LNP = 0.
 
double Cquqd8_3121r_LNP = 0.
 
double Cquqd8_3122i_LNP = 0.
 
double Cquqd8_3122r_LNP = 0.
 
double Cquqd8_3123i_LNP = 0.
 
double Cquqd8_3123r_LNP = 0.
 
double Cquqd8_3131i_LNP = 0.
 
double Cquqd8_3131r_LNP = 0.
 
double Cquqd8_3132i_LNP = 0.
 
double Cquqd8_3132r_LNP = 0.
 
double Cquqd8_3133i_LNP = 0.
 
double Cquqd8_3133r_LNP = 0.
 
double Cquqd8_3211i_LNP = 0.
 
double Cquqd8_3211r_LNP = 0.
 
double Cquqd8_3212i_LNP = 0.
 
double Cquqd8_3212r_LNP = 0.
 
double Cquqd8_3213i_LNP = 0.
 
double Cquqd8_3213r_LNP = 0.
 
double Cquqd8_3221i_LNP = 0.
 
double Cquqd8_3221r_LNP = 0.
 
double Cquqd8_3222i_LNP = 0.
 
double Cquqd8_3222r_LNP = 0.
 
double Cquqd8_3223i_LNP = 0.
 
double Cquqd8_3223r_LNP = 0.
 
double Cquqd8_3231i_LNP = 0.
 
double Cquqd8_3231r_LNP = 0.
 
double Cquqd8_3232i_LNP = 0.
 
double Cquqd8_3232r_LNP = 0.
 
double Cquqd8_3233i_LNP = 0.
 
double Cquqd8_3233r_LNP = 0.
 
double Cquqd8_3311i_LNP = 0.
 
double Cquqd8_3311r_LNP = 0.
 
double Cquqd8_3312i_LNP = 0.
 
double Cquqd8_3312r_LNP = 0.
 
double Cquqd8_3313i_LNP = 0.
 
double Cquqd8_3313r_LNP = 0.
 
double Cquqd8_3321i_LNP = 0.
 
double Cquqd8_3321r_LNP = 0.
 
double Cquqd8_3322i_LNP = 0.
 
double Cquqd8_3322r_LNP = 0.
 
double Cquqd8_3323i_LNP = 0.
 
double Cquqd8_3323r_LNP = 0.
 
double Cquqd8_3331i_LNP = 0.
 
double Cquqd8_3331r_LNP = 0.
 
double Cquqd8_3332i_LNP = 0.
 
double Cquqd8_3332r_LNP = 0.
 
double Cquqd8_3333i_LNP = 0.
 The dimension-6 operator coefficient \((C_{quqd}^{(8)})_{ijkm}\) (Imaginary part). More...
 
double Cquqd8_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{quqd}^{(8)})_{ijkm}\) (Real part and pure real operator). More...
 
double CuB_11i_LNP = 0.
 
double CuB_11r_LNP = 0.
 
double CuB_12i_LNP = 0.
 
double CuB_12r_LNP = 0.
 
double CuB_13i_LNP = 0.
 
double CuB_13r_LNP = 0.
 
double CuB_21i_LNP = 0.
 
double CuB_21r_LNP = 0.
 
double CuB_22i_LNP = 0.
 
double CuB_22r_LNP = 0.
 
double CuB_23i_LNP = 0.
 
double CuB_23r_LNP = 0.
 
double CuB_31i_LNP = 0.
 
double CuB_31r_LNP = 0.
 
double CuB_32i_LNP = 0.
 
double CuB_32r_LNP = 0.
 
double CuB_33i_LNP = 0.
 The dimension-6 operator coefficient \((C_{uB})_{ij}\) (Imaginary part). More...
 
double CuB_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{uB})_{ij}\) (Real part and pure real operator). More...
 
double Cud1_1111r_LNP = 0.
 
double Cud1_1112i_LNP = 0.
 
double Cud1_1112r_LNP = 0.
 
double Cud1_1113i_LNP = 0.
 
double Cud1_1113r_LNP = 0.
 
double Cud1_1122r_LNP = 0.
 
double Cud1_1123i_LNP = 0.
 
double Cud1_1123r_LNP = 0.
 
double Cud1_1133r_LNP = 0.
 
double Cud1_1211i_LNP = 0.
 
double Cud1_1211r_LNP = 0.
 
double Cud1_1212i_LNP = 0.
 
double Cud1_1212r_LNP = 0.
 
double Cud1_1213i_LNP = 0.
 
double Cud1_1213r_LNP = 0.
 
double Cud1_1221i_LNP = 0.
 
double Cud1_1221r_LNP = 0.
 
double Cud1_1222i_LNP = 0.
 
double Cud1_1222r_LNP = 0.
 
double Cud1_1223i_LNP = 0.
 
double Cud1_1223r_LNP = 0.
 
double Cud1_1231i_LNP = 0.
 
double Cud1_1231r_LNP = 0.
 
double Cud1_1232i_LNP = 0.
 
double Cud1_1232r_LNP = 0.
 
double Cud1_1233i_LNP = 0.
 
double Cud1_1233r_LNP = 0.
 
double Cud1_1311i_LNP = 0.
 
double Cud1_1311r_LNP = 0.
 
double Cud1_1312i_LNP = 0.
 
double Cud1_1312r_LNP = 0.
 
double Cud1_1313i_LNP = 0.
 
double Cud1_1313r_LNP = 0.
 
double Cud1_1321i_LNP = 0.
 
double Cud1_1321r_LNP = 0.
 
double Cud1_1322i_LNP = 0.
 
double Cud1_1322r_LNP = 0.
 
double Cud1_1323i_LNP = 0.
 
double Cud1_1323r_LNP = 0.
 
double Cud1_1331i_LNP = 0.
 
double Cud1_1331r_LNP = 0.
 
double Cud1_1332i_LNP = 0.
 
double Cud1_1332r_LNP = 0.
 
double Cud1_1333i_LNP = 0.
 
double Cud1_1333r_LNP = 0.
 
double Cud1_2211r_LNP = 0.
 
double Cud1_2212i_LNP = 0.
 
double Cud1_2212r_LNP = 0.
 
double Cud1_2213i_LNP = 0.
 
double Cud1_2213r_LNP = 0.
 
double Cud1_2222r_LNP = 0.
 
double Cud1_2223i_LNP = 0.
 
double Cud1_2223r_LNP = 0.
 
double Cud1_2233r_LNP = 0.
 
double Cud1_2311i_LNP = 0.
 
double Cud1_2311r_LNP = 0.
 
double Cud1_2312i_LNP = 0.
 
double Cud1_2312r_LNP = 0.
 
double Cud1_2313i_LNP = 0.
 
double Cud1_2313r_LNP = 0.
 
double Cud1_2321i_LNP = 0.
 
double Cud1_2321r_LNP = 0.
 
double Cud1_2322i_LNP = 0.
 
double Cud1_2322r_LNP = 0.
 
double Cud1_2323i_LNP = 0.
 
double Cud1_2323r_LNP = 0.
 
double Cud1_2331i_LNP = 0.
 
double Cud1_2331r_LNP = 0.
 
double Cud1_2332i_LNP = 0.
 
double Cud1_2332r_LNP = 0.
 
double Cud1_2333i_LNP = 0.
 
double Cud1_2333r_LNP = 0.
 
double Cud1_3311r_LNP = 0.
 
double Cud1_3312i_LNP = 0.
 
double Cud1_3312r_LNP = 0.
 
double Cud1_3313i_LNP = 0.
 
double Cud1_3313r_LNP = 0.
 
double Cud1_3322r_LNP = 0.
 
double Cud1_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{ud}^{(1)})_{ijkm}\) (Imaginary part). More...
 
double Cud1_3323r_LNP = 0.
 
double Cud1_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{ud}^{(1)})_{ijkm}\) (Real part and pure real operator). More...
 
double Cud8_1111r_LNP = 0.
 
double Cud8_1112i_LNP = 0.
 
double Cud8_1112r_LNP = 0.
 
double Cud8_1113i_LNP = 0.
 
double Cud8_1113r_LNP = 0.
 
double Cud8_1122r_LNP = 0.
 
double Cud8_1123i_LNP = 0.
 
double Cud8_1123r_LNP = 0.
 
double Cud8_1133r_LNP = 0.
 
double Cud8_1211i_LNP = 0.
 
double Cud8_1211r_LNP = 0.
 
double Cud8_1212i_LNP = 0.
 
double Cud8_1212r_LNP = 0.
 
double Cud8_1213i_LNP = 0.
 
double Cud8_1213r_LNP = 0.
 
double Cud8_1221i_LNP = 0.
 
double Cud8_1221r_LNP = 0.
 
double Cud8_1222i_LNP = 0.
 
double Cud8_1222r_LNP = 0.
 
double Cud8_1223i_LNP = 0.
 
double Cud8_1223r_LNP = 0.
 
double Cud8_1231i_LNP = 0.
 
double Cud8_1231r_LNP = 0.
 
double Cud8_1232i_LNP = 0.
 
double Cud8_1232r_LNP = 0.
 
double Cud8_1233i_LNP = 0.
 
double Cud8_1233r_LNP = 0.
 
double Cud8_1311i_LNP = 0.
 
double Cud8_1311r_LNP = 0.
 
double Cud8_1312i_LNP = 0.
 
double Cud8_1312r_LNP = 0.
 
double Cud8_1313i_LNP = 0.
 
double Cud8_1313r_LNP = 0.
 
double Cud8_1321i_LNP = 0.
 
double Cud8_1321r_LNP = 0.
 
double Cud8_1322i_LNP = 0.
 
double Cud8_1322r_LNP = 0.
 
double Cud8_1323i_LNP = 0.
 
double Cud8_1323r_LNP = 0.
 
double Cud8_1331i_LNP = 0.
 
double Cud8_1331r_LNP = 0.
 
double Cud8_1332i_LNP = 0.
 
double Cud8_1332r_LNP = 0.
 
double Cud8_1333i_LNP = 0.
 
double Cud8_1333r_LNP = 0.
 
double Cud8_2211r_LNP = 0.
 
double Cud8_2212i_LNP = 0.
 
double Cud8_2212r_LNP = 0.
 
double Cud8_2213i_LNP = 0.
 
double Cud8_2213r_LNP = 0.
 
double Cud8_2222r_LNP = 0.
 
double Cud8_2223i_LNP = 0.
 
double Cud8_2223r_LNP = 0.
 
double Cud8_2233r_LNP = 0.
 
double Cud8_2311i_LNP = 0.
 
double Cud8_2311r_LNP = 0.
 
double Cud8_2312i_LNP = 0.
 
double Cud8_2312r_LNP = 0.
 
double Cud8_2313i_LNP = 0.
 
double Cud8_2313r_LNP = 0.
 
double Cud8_2321i_LNP = 0.
 
double Cud8_2321r_LNP = 0.
 
double Cud8_2322i_LNP = 0.
 
double Cud8_2322r_LNP = 0.
 
double Cud8_2323i_LNP = 0.
 
double Cud8_2323r_LNP = 0.
 
double Cud8_2331i_LNP = 0.
 
double Cud8_2331r_LNP = 0.
 
double Cud8_2332i_LNP = 0.
 
double Cud8_2332r_LNP = 0.
 
double Cud8_2333i_LNP = 0.
 
double Cud8_2333r_LNP = 0.
 
double Cud8_3311r_LNP = 0.
 
double Cud8_3312i_LNP = 0.
 
double Cud8_3312r_LNP = 0.
 
double Cud8_3313i_LNP = 0.
 
double Cud8_3313r_LNP = 0.
 
double Cud8_3322r_LNP = 0.
 
double Cud8_3323i_LNP = 0.
 The dimension-6 operator coefficient \((C_{ud}^{(8)})_{ijkm}\) (Imaginary part). More...
 
double Cud8_3323r_LNP = 0.
 
double Cud8_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{ud}^{(8)})_{ijkm}\) (Real part and pure real operator). More...
 
double CuG_11i_LNP = 0.
 
double CuG_11r_LNP = 0.
 
double CuG_12i_LNP = 0.
 
double CuG_12r_LNP = 0.
 
double CuG_13i_LNP = 0.
 
double CuG_13r_LNP = 0.
 
double CuG_21i_LNP = 0.
 
double CuG_21r_LNP = 0.
 
double CuG_22i_LNP = 0.
 
double CuG_22r_LNP = 0.
 
double CuG_23i_LNP = 0.
 
double CuG_23r_LNP = 0.
 
double CuG_31i_LNP = 0.
 
double CuG_31r_LNP = 0.
 
double CuG_32i_LNP = 0.
 
double CuG_32r_LNP = 0.
 
double CuG_33i_LNP = 0.
 The dimension-6 operator coefficient \((C_{uG})_{ij}\) (Imaginary part). More...
 
double CuG_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{uG})_{ij}\) (Real part and pure real operator). More...
 
double CuH_11i_LNP = 0.
 
double CuH_11r_LNP = 0.
 
double CuH_12i_LNP = 0.
 
double CuH_12r_LNP = 0.
 
double CuH_13i_LNP = 0.
 
double CuH_13r_LNP = 0.
 
double CuH_21i_LNP = 0.
 
double CuH_21r_LNP = 0.
 
double CuH_22i_LNP = 0.
 
double CuH_22r_LNP = 0.
 
double CuH_23i_LNP = 0.
 
double CuH_23r_LNP = 0.
 
double CuH_31i_LNP = 0.
 
double CuH_31r_LNP = 0.
 
double CuH_32i_LNP = 0.
 
double CuH_32r_LNP = 0.
 
double CuH_33i_LNP = 0.
 The dimension-6 operator coefficient \((C_{uH})_{ij}\) (Imaginary part). More...
 
double CuH_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{uH})_{ij}\) (Real part and pure real operator). More...
 
double Cuu_1111r_LNP = 0.
 
double Cuu_1112i_LNP = 0.
 
double Cuu_1112r_LNP = 0.
 
double Cuu_1113i_LNP = 0.
 
double Cuu_1113r_LNP = 0.
 
double Cuu_1122r_LNP = 0.
 
double Cuu_1123i_LNP = 0.
 
double Cuu_1123r_LNP = 0.
 
double Cuu_1133r_LNP = 0.
 
double Cuu_1212i_LNP = 0.
 
double Cuu_1212r_LNP = 0.
 
double Cuu_1213i_LNP = 0.
 
double Cuu_1213r_LNP = 0.
 
double Cuu_1221r_LNP = 0.
 
double Cuu_1222i_LNP = 0.
 
double Cuu_1222r_LNP = 0.
 
double Cuu_1223i_LNP = 0.
 
double Cuu_1223r_LNP = 0.
 
double Cuu_1231i_LNP = 0.
 
double Cuu_1231r_LNP = 0.
 
double Cuu_1232i_LNP = 0.
 
double Cuu_1232r_LNP = 0.
 
double Cuu_1233i_LNP = 0.
 
double Cuu_1233r_LNP = 0.
 
double Cuu_1313i_LNP = 0.
 
double Cuu_1313r_LNP = 0.
 
double Cuu_1322i_LNP = 0.
 
double Cuu_1322r_LNP = 0.
 
double Cuu_1323i_LNP = 0.
 
double Cuu_1323r_LNP = 0.
 
double Cuu_1331r_LNP = 0.
 
double Cuu_1332i_LNP = 0.
 
double Cuu_1332r_LNP = 0.
 
double Cuu_1333i_LNP = 0.
 
double Cuu_1333r_LNP = 0.
 
double Cuu_2222r_LNP = 0.
 
double Cuu_2223i_LNP = 0.
 
double Cuu_2223r_LNP = 0.
 
double Cuu_2233r_LNP = 0.
 
double Cuu_2323i_LNP = 0.
 
double Cuu_2323r_LNP = 0.
 
double Cuu_2332r_LNP = 0.
 
double Cuu_2333i_LNP = 0.
 The dimension-6 operator coefficient \((C_{uu})_{ijkm}\) (Imaginary part). More...
 
double Cuu_2333r_LNP = 0.
 
double Cuu_3333r_LNP = 0.
 The dimension-6 operator coefficient \((C_{uu})_{ijkm}\) (Real part and pure real operator). More...
 
double CuW_11i_LNP = 0.
 
double CuW_11r_LNP = 0.
 
double CuW_12i_LNP = 0.
 
double CuW_12r_LNP = 0.
 
double CuW_13i_LNP = 0.
 
double CuW_13r_LNP = 0.
 
double CuW_21i_LNP = 0.
 
double CuW_21r_LNP = 0.
 
double CuW_22i_LNP = 0.
 
double CuW_22r_LNP = 0.
 
double CuW_23i_LNP = 0.
 
double CuW_23r_LNP = 0.
 
double CuW_31i_LNP = 0.
 
double CuW_31r_LNP = 0.
 
double CuW_32i_LNP = 0.
 
double CuW_32r_LNP = 0.
 
double CuW_33i_LNP = 0.
 The dimension-6 operator coefficient \((C_{uW})_{ij}\) (Imaginary part). More...
 
double CuW_33r_LNP = 0.
 The dimension-6 operator coefficient \((C_{uW})_{ij}\) (Real part and pure real operator). More...
 
double cW2_tree
 The square of the tree level values for the cosine of the weak angle. More...
 
double CW_LNP = 0.
 The dimension-6 operator coefficient \(C_{W}\). More...
 
double cW_tree
 The tree level values for the cosine of the weak angle. More...
 
double cWsch
 Parameters to control the SM EW input scheme: Alpha or MW. More...
 
double CWtilde_LNP = 0.
 The dimension-6 operator coefficient \(C_{\tilde{W}}\). More...
 
double dCKM_LEW = 0.
 
double delta_A
 Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition for EWPO. More...
 
double delta_AA
 Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More...
 
double delta_ale
 The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the electromagnetic coupling. More...
 
double delta_ale_2
 The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the electromagnetic coupling. More...
 
double delta_AZ
 Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More...
 
double delta_e
 The dimension 6 correction to the electric constant parameter. More...
 
double delta_em
 The relative dimension 6 correction to the QED interaction vertex. More...
 
double delta_g1
 The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the \(U(1)_Y\) gauge coupling, for the Alpha-Scheme (cAsch=1, cWsch=0) or the Mw-Scheme (cAsch=0, cWsch=1). More...
 
double delta_g1_2
 The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the \(U(1)_Y\) gauge coupling. More...
 
double delta_g2
 The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the \(SU(2)_L\) gauge coupling, for the Alpha-Scheme (cAsch=1, cWsch=0) or the Mw-Scheme (cAsch=0, cWsch=1). More...
 
double delta_g2_2
 The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the \(SU(2)_L\) gauge coupling. More...
 
double delta_GF
 The dimension 6 correction to the Fermi constant, as extracted from muon decay. More...
 
double delta_GF_2
 The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the Fermi constant. More...
 
double delta_h
 Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition. More...
 
double delta_MW
 The dimension 6 correction to W mass Lagrangian parameter. More...
 
double delta_MZ
 The dimension 6 correction to Z mass Lagrangian parameter. More...
 
double delta_Mz2
 The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the Z-boson mass squared. More...
 
double delta_Mz2_2
 The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the Z-boson mass squared. More...
 
double delta_QgNC
 The dimension 6 charge correction to neutral current EW couplings. More...
 
double delta_sW2
 The dimension 6 correction to the weak mixing angle. More...
 
double delta_UgCC
 The dimension 6 universal correction to charged current EW couplings. More...
 
double delta_UgNC
 The dimension 6 universal correction to neutral current EW couplings. More...
 
double delta_v
 The dimension 6 correction to the vev, as extracted from GF. More...
 
double delta_xBZ
 The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the component of the matrix that transform the gauge field \(B_{\mu}\) into \(Z_{\mu}\). More...
 
double delta_xBZ_2
 The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the component of the matrix that transform the gauge field \(B_{\mu}\) into \(Z_{\mu}\). More...
 
double delta_xWZ
 The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the component of the matrix that transform the gauge field \(W_{\mu}^3\) into \(Z_{\mu}\). More...
 
double delta_xWZ_2
 The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the component of the matrix that transform the gauge field \(W_{\mu}^3\) into \(Z_{\mu}\). More...
 
double delta_Z
 Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition for EWPO. More...
 
double delta_ZA
 Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition for EWPO. More...
 
double delta_ZZ
 Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition. More...
 
double dGammaHTotR1
 
double dGammaHTotR2
 
double dZH
 
double dZH1
 
double dZH2
 Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization and combinations entering in the linear and quadratic pieces. More...
 
double edeeWWdcint = 0.
 Intrinsic relative theoretical error in \(e^+ e^- \to W^+ W^-\): total cross section and \(d/d\cos{\theta}\) distribution. More...
 
double eeettHint = 0.
 Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More...
 
double eeettHpar = 0.
 Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More...
 
double eeeWBFint = 0.
 Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More...
 
double eeeWBFpar = 0.
 Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More...
 
double eeeWWint = 0.
 
double eeeZHint = 0.
 Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More...
 
double eeeZHpar = 0.
 Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More...
 
double eeMz
 The em coupling at Mz. More...
 
double eeMz2
 The em coupling squared (at Mz). More...
 
double eepWBFint = 0.
 Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.) More...
 
double eepWBFpar = 0.
 Parametric relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.)
More...
 
double eepZBFint = 0.
 Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.) More...
 
double eepZBFpar = 0.
 Parametric relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.) More...
 
double eggFHbb = 0.
 
double eggFHgaga = 0.
 
double eggFHmumu = 0.
 Total relative theoretical error in \(gg \to H \to X\).
More...
 
double eggFHtautau = 0.
 
double eggFHWW = 0.
 
double eggFHZga = 0.
 
double eggFHZZ = 0.
 
double eggFint = 0.
 Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.) More...
 
double eggFpar = 0.
 Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.) More...
 
double eHbbint = 0.
 Intrinsic relative theoretical error in \(H \to b\bar{b}\). More...
 
double eHbbpar = 0.
 Parametric relative theoretical error in \(H \to b\bar{b}\). More...
 
double eHccint = 0.
 Intrinsic relative theoretical error in \(H \to c\bar{c}\). More...
 
double eHccpar = 0.
 Parametric relative theoretical error in \(H \to c\bar{c}\). More...
 
double eHgagaint = 0.
 Intrinsic relative theoretical error in \(H \to \gamma\gamma\). More...
 
double eHgagapar = 0.
 Parametric relative theoretical error in \(H \to \gamma\gamma\). More...
 
double eHggint = 0.
 Intrinsic relative theoretical error in \(H \to g g\). More...
 
double eHggpar = 0.
 Parametric relative theoretical error in \(H \to g g\). More...
 
double eHmumuint = 0.
 Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\). More...
 
double eHmumupar = 0.
 Parametric relative theoretical error in \(H \to \mu^+ \mu^-\). More...
 
double eHssint = 0.
 Intrinsic relative theoretical error in \(H \to s\bar{s}\). More...
 
double eHsspar = 0.
 Parametric relative theoretical error in \(H \to s\bar{s}\). More...
 
double eHtautauint = 0.
 Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\). More...
 
double eHtautaupar = 0.
 Parametric relative theoretical error in \(H \to \tau^+ \tau^-\). More...
 
double eHwidth = 0.
 Total relative theoretical error in the Higgs width. More...
 
double eHWWint = 0.
 Intrinsic relative theoretical error in \(H \to W W\). More...
 
double eHWWpar = 0.
 Parametric relative theoretical error in \(H \to W W\). More...
 
double eHZgaint = 0.
 Intrinsic relative theoretical error in \(H \to Z \gamma\). More...
 
double eHZgapar = 0.
 Parametric relative theoretical error in \(H \to Z \gamma\). More...
 
double eHZZint = 0.
 Intrinsic relative theoretical error in \(H \to Z Z\). More...
 
double eHZZpar = 0.
 Parametric relative theoretical error in \(H \to Z Z\). More...
 
double ettHbb = 0.
 
double ettHgaga = 0.
 
double ettHint = 0.
 Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.) More...
 
double ettHmumu = 0.
 Total relative theoretical error in \(pp \to ttH \to tt X\). More...
 
double ettHpar = 0.
 Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.) More...
 
double ettHtautau = 0.
 
double ettHWW = 0.
 
double ettHZga = 0.
 
double ettHZZ = 0.
 
double eVBFHbb = 0.
 
double eVBFHgaga = 0.
 
double eVBFHinv = 0.
 
double eVBFHmumu = 0.
 Total relative theoretical error in \(pp \to Hjj (VBF) \to X jj\).
More...
 
double eVBFHtautau = 0.
 
double eVBFHWW = 0.
 
double eVBFHZga = 0.
 
double eVBFHZZ = 0.
 
double eVBFint = 0.
 Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.) More...
 
double eVBFpar = 0.
 Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.) More...
 
double eVHinv = 0.
 Total relative theoretical error in \(pp \to X H \to X + invisible\). More...
 
double eWHbb = 0.
 
double eWHgaga = 0.
 
double eWHint = 0.
 Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.) More...
 
double eWHmumu = 0.
 Total relative theoretical error in \(pp \to WH \to W X\).
More...
 
double eWHpar = 0.
 Parametric relative theoretical error in WH production. (Assumed to be constant in energy.) More...
 
double eWHtautau = 0.
 
double eWHWW = 0.
 
double eWHZga = 0.
 
double eWHZZ = 0.
 
double eZHbb = 0.
 
double eZHgaga = 0.
 
double eZHint = 0.
 Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.) More...
 
double eZHmumu = 0.
 Total relative theoretical error in \(pp \to ZH \to Z X\). More...
 
double eZHpar = 0.
 Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.) More...
 
double eZHtautau = 0.
 
double eZHWW = 0.
 
double eZHZga = 0.
 
double eZHZZ = 0.
 
int flavBas = 1
 
double g1_LEW = 0
 
double g1_tree
 The tree level value of the \(U(1)_Y\) gauge coupling contant (at the \(Z\) pole). More...
 
double g2_LEW = 0
 
double g2_tree
 The tree level value of the \(SU(2)_L\) gauge coupling contant (at the \(Z\) pole). More...
 
double g3_LEW = 0
 
double g3_tree
 The tree level value of the \(SU(3)_c\) gauge coupling contant (at the \(Z\) pole). More...
 
double GammaHTotR
 NP contributions and Total to Higgs width ratio with SM. More...
 
double gZdL
 
double gZdR
 The tree level value of the \(Z\bar{d}d\) couplings in the SM. More...
 
double gZlL
 
double gZlR
 The tree level value of the \(Z\ell^+\ell^-\) couplings in the SM. More...
 
double gZuL
 
double gZuR
 The tree level value of the \(Z\bar{u}u\) couplings in the SM. More...
 
double gZvL
 The tree level value of the \(Z\bar{\nu}\nu\) couplings in the SM. More...
 
double Lambda_NP
 The new physics scale [GeV]. More...
 
double lambdaH_LEW = 0
 
double lambdaH_tree
 The SM tree level value of the scalar quartic coupling in the potential. More...
 
double LambdaNP2
 The square of the new physics scale [GeV \(^2\)]. More...
 
double LambdaNPm2
 The inverse square of the new physics scale [GeV \(^{-2}\)]. More...
 
double mb_LEW = 0
 
double mc_LEW = 0
 
double md_LEW = 0
 
double Md_LEW [3] = {0, 0, 0}
 
double me_LEW = 0
 
double Me_LEW [3] = {0, 0, 0}
 
double mH2_LEW = 0
 
double mmu_LEW = 0
 
double ms_LEW = 0
 
double mt_LEW = 0
 
double mtau_LEW = 0
 
double mu_LEW = 0
 
double Mu_LEW [3] = {0, 0, 0}
 
double Mw_tree
 The tree level value of the \(W\) boson mass. More...
 
Matching< NPSMEFTd6GeneralMatching, NPSMEFTd6GeneralNPSMEFTd6GM
 An auxiliary method to get the WC from the evolutor. More...
 
double s12CKM_LEW = 0.
 
double s13CKM_LEW = 0.
 
double s23CKM_LEW = 0.
 
std::string SMEFTBasisFlag
 
RGESolver SMEFTEvol1000
 
RGESolver SMEFTEvol1500
 
RGESolver SMEFTEvol240
 
RGESolver SMEFTEvol3000
 
RGESolver SMEFTEvol365
 
RGESolver SMEFTEvol5000
 
RGESolver SMEFTEvol550
 
RGESolver SMEFTEvolEW
 
RGESolver SMEFTEvolMH
 
RGESolver SMEFTEvolUV
 
double sW2_tree
 The square of the tree level values for the sine of the weak angle. More...
 
double sW_tree
 The tree level values for the sine of the weak angle. More...
 
double tmu2 = 0.
 
double tmu3 = 0.
 
double tmu4 = 0.
 
double tmu5 = 0.
 
double tmuw = 0.
 
double UevL
 The tree level value of the \(W^-\bar{\ell}\nu\) couplings in the SM. (Neglecting PMNS effects.) More...
 
double v2
 The square of the EW vev. More...
 
double v2_over_LambdaNP2
 The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\). More...
 
double VudL
 The tree level value of the \(W^+\bar{u}d\) couplings in the SM. (Neglecting CKM effects.) More...
 
double xBZ_tree
 The tree level component of the matrix that transform the gauge field \(B_{\mu}\) into \(Z_{\mu}\). More...
 
double xWZ_tree
 The tree level component of the matrix that transform the gauge field \(W_{\mu}^3\) into \(Z_{\mu}\). More...
 
double Yukc
 
double Yukt
 SM u-quark Yukawas. More...
 
double Yuku
 
- Protected Attributes inherited from NPbase
StandardModel trueSM
 
- Protected Attributes inherited from StandardModel
double A
 The CKM parameter \(A\) in the Wolfenstein parameterization. More...
 
double ale
 The fine-structure constant \(\alpha\). More...
 
double alpha21
 
double alpha31
 
double AlsMz
 The strong coupling constant at the Z-boson mass, \(\alpha_s(M_Z)\). More...
 
bool bSigmaForAFB
 
bool bSigmaForR
 
double dAl5hMz
 The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). (Non-input parameter) More...
 
double dAle5Mz
 The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\), used as input for FlagMWinput = FALSE. More...
 
double delGammaWlv
 The theoretical uncertainty in \(\Gamma_W_{l\nu}\), denoted as \(\delta\,\Gamma_W_{l\nu}\). More...
 
double delGammaWqq
 The theoretical uncertainty in \(\Gamma_W_{qq}\), denoted as \(\delta\,\Gamma_W_{qq}\). More...
 
double delGammaZ
 The theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\), in GeV. More...
 
double delMw
 The theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\), in GeV. More...
 
double delR0b
 The theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More...
 
double delR0c
 The theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More...
 
double delR0l
 The theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More...
 
double delsigma0H
 The theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\) in nb. More...
 
double delSin2th_b
 The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More...
 
double delSin2th_l
 The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More...
 
double delSin2th_q
 The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More...
 
double delta
 
double etab
 The CKM parameter \(\bar{\eta}\) in the Wolfenstein parameterization. More...
 
bool flag_order [orders_EW_size]
 An array of internal flags controlling the inclusions of higher-order corrections. More...
 
bool FlagFixMuwMut
 A boolean for the model flag FixMuwMut. More...
 
bool flagLEP2 [NUMofLEP2RCs]
 
double gamma
 \(\gamma \) used as an input for FlagWolfenstein = FALSE More...
 
double GF
 The Fermi constant \(G_\mu\) in \({\rm GeV}^{-2}\). More...
 
double lambda
 The CKM parameter \(\lambda\) in the Wolfenstein parameterization. More...
 
Particle leptons [6]
 An array of Particle objects for the leptons. More...
 
double mHl
 The Higgs mass \(m_h\) in GeV. More...
 
double muw
 A matching scale \(\mu_W\) around the weak scale in GeV. More...
 
double Mw_inp
 The mass of the \(W\) boson in GeV used as input for FlagMWinput = TRUE. More...
 
CKM myCKM
 An object of type CKM. More...
 
PMNS myPMNS
 
double Mz
 The mass of the \(Z\) boson in GeV. More...
 
bool requireCKM
 An internal flag to control whether the CKM matrix has to be recomputed. More...
 
bool requireYe
 An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed. More...
 
bool requireYn
 An internal flag to control whether the neutrino Yukawa matrix has to be recomputed. More...
 
double rhob
 The CKM parameter \(\bar{\rho}\) in the Wolfenstein parameterization. More...
 
double s12
 
double s13
 
double s23
 
Flavour SMFlavour
 An object of type Flavour. More...
 
Matching< StandardModelMatching, StandardModelSMM
 An object of type Matching. More...
 
double Vcb
 \(\vert V_{cb} \vert \) used as an input for FlagWolfenstein = FALSE More...
 
double Vub
 \(\vert V_{ub} \vert \) used as an input for FlagWolfenstein = FALSE More...
 
double Vud
 \(\vert V_{ud} \vert \) used as an input for FlagWolfenstein = FALSE and FlagUseVud = TRUE More...
 
double Vus
 \(\vert V_{us} \vert \) used as an input for FlagWolfenstein = FALSE More...
 
gslpp::matrix< gslpp::complex > Yd
 The Yukawa matrix of the down-type quarks. More...
 
gslpp::matrix< gslpp::complex > Ye
 The Yukawa matrix of the charged leptons. More...
 
gslpp::matrix< gslpp::complex > Yn
 The Yukawa matrix of the neutrinos. More...
 
gslpp::matrix< gslpp::complex > Yu
 The Yukawa matrix of the up-type quarks. More...
 
- Protected Attributes inherited from QCD
double AlsM
 The strong coupling constant at the mass scale MAls, \(\alpha_s(M_{\alpha_s})\). More...
 
double CA
 
double CF
 
bool computemt
 Switch for computing the \(\overline{\mathrm{MS}}\) mass of the top quark. More...
 
double dAdA_NA
 
double dFdA_NA
 
double dFdF_NA
 
bool FlagMpole2MbarNumeric
 A flag to determine whether the pole mass to \(\over \mathrm{MS}\) mass conversion is done numerically. More...
 
bool FlagMtPole
 A flag to determine whether the pole mass of the top quark is used as input. More...
 
double MAls
 The mass scale in GeV at which the strong coupling measurement is provided. More...
 
double mtpole
 The pole mass of the top quark. More...
 
double mub
 The threshold between five- and four-flavour theory in GeV. More...
 
double muc
 The threshold between four- and three-flavour theory in GeV. More...
 
double mut
 The threshold between six- and five-flavour theory in GeV. More...
 
double NA
 
double Nc
 The number of colours. More...
 
bool QCDsuccess =true
 
Particle quarks [6]
 The vector of all SM quarks. More...
 
bool requireYd
 Switch for generating the Yukawa couplings to the down-type quarks. More...
 
bool requireYu
 Switch for generating the Yukawa couplings to the up-type quarks. More...
 
double TF
 
- Protected Attributes inherited from Model
bool isSliced = false
 A boolean set to true if the current istance is a slice of an extended object. More...
 
std::map< std::string, std::reference_wrapper< const double > > ModelParamMap
 
bool UpdateError = false
 A boolean set to false if update is successful. More...
 

Additional Inherited Members

- Public Types inherited from StandardModel
enum  LEP2RCs { Weak = 0 , WeakBox , ISR , QEDFSR , QCDFSR , NUMofLEP2RCs }
 
enum  orders_EW { EW1 = 0 , EW1QCD1 , EW1QCD2 , EW2 , EW2QCD1 , EW3 , orders_EW_size }
 An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More...
 
- Public Types inherited from QCD
enum  lepton { NEUTRINO_1 , ELECTRON , NEUTRINO_2 , MU , NEUTRINO_3 , TAU , NOLEPTON }
 An enum type for leptons. More...
 
enum  meson { P_0 , P_P , K_0 , K_P , D_0 , D_P , D_S , B_D , B_P , B_S , B_C , PHI , K_star , K_star_P , K_S , D_star_P , RHO , RHO_P , OMEGA , MESON_END }
 An enum type for mesons. More...
 
enum  quark { UP , DOWN , CHARM , STRANGE , TOP , BOTTOM }
 An enum type for quarks. More...
 
- Public Attributes inherited from NPSMEFTd6General
bool FlagNewTerms
 A boolean for the model flag NewTerms, to include corrections in the matching between SMEFT and LEFT. More...
 
- Public Attributes inherited from NPbase
double C1Hbb = 0.0
 
double C1Hcc = 0.0
 
double C1Hgaga = 0.0049
 
double C1Hgg = 0.0066
 
double C1Hmumu = 0.0
 The C1 coefficient controlling the H^3 corrections to the Higgs partial width from the Higgs trilinear coupling. More...
 
double C1Hss = 0.0
 
double C1Htautau = 0.0
 
double C1HWW = 0.0073
 
double C1HZga = 0.0
 The C1 coefficient controlling the H^3 corrections to the Higgs partial width from the Higgs trilinear coupling.
More...
 
double C1HZZ = 0.0083
 

Constructor & Destructor Documentation

◆ NPSMEFTd6MFV()

NPSMEFTd6MFV::NPSMEFTd6MFV ( )

Definition at line 35 of file NPSMEFTd6MFV.cpp.

36 setModelName("NPSMEFTd6MFV");
37 ModelParamMap.insert(std::make_pair("CG_LNP",std::cref(CG_LNP)));
38 ModelParamMap.insert(std::make_pair("CW_LNP",std::cref(CW_LNP)));
39 ModelParamMap.insert(std::make_pair("CHG_LNP",std::cref(CHG_LNP)));
40 ModelParamMap.insert(std::make_pair("CHW_LNP",std::cref(CHW_LNP)));
41 ModelParamMap.insert(std::make_pair("CHB_LNP",std::cref(CHB_LNP)));
42 ModelParamMap.insert(std::make_pair("CHWB_LNP",std::cref(CHWB_LNP)));
43 ModelParamMap.insert(std::make_pair("CHD_LNP",std::cref(CHD_LNP)));
44 ModelParamMap.insert(std::make_pair("CHbox_LNP",std::cref(CHbox_LNP)));
45 ModelParamMap.insert(std::make_pair("CH_LNP",std::cref(CH_LNP)));
46 ModelParamMap.insert(std::make_pair("CHl1_LNP",std::cref(CHl1_LNP)));
47 ModelParamMap.insert(std::make_pair("CHl3_LNP",std::cref(CHl3_LNP)));
48 ModelParamMap.insert(std::make_pair("CHe_LNP",std::cref(CHe_LNP)));
49 ModelParamMap.insert(std::make_pair("Cll_aabb_LNP",std::cref(Cll_aabb_LNP)));
50 ModelParamMap.insert(std::make_pair("Cll_abba_LNP",std::cref(Cll_abba_LNP)));
51 ModelParamMap.insert(std::make_pair("Cee_LNP",std::cref(Cee_LNP)));
52 ModelParamMap.insert(std::make_pair("Cle_LNP",std::cref(Cle_LNP)));
53 ModelParamMap.insert(std::make_pair("CuH_0_LNP",std::cref(CuH_0_LNP)));
54 ModelParamMap.insert(std::make_pair("CuH_u_LNP",std::cref(CuH_u_LNP)));
55 ModelParamMap.insert(std::make_pair("CuH_d_LNP",std::cref(CuH_d_LNP)));
56 ModelParamMap.insert(std::make_pair("CuG_0_LNP",std::cref(CuG_0_LNP)));
57 ModelParamMap.insert(std::make_pair("CuG_u_LNP",std::cref(CuG_u_LNP)));
58 ModelParamMap.insert(std::make_pair("CuG_d_LNP",std::cref(CuG_d_LNP)));
59 ModelParamMap.insert(std::make_pair("CuW_0_LNP",std::cref(CuW_0_LNP)));
60 ModelParamMap.insert(std::make_pair("CuW_u_LNP",std::cref(CuW_u_LNP)));
61 ModelParamMap.insert(std::make_pair("CuW_d_LNP",std::cref(CuW_d_LNP)));
62 ModelParamMap.insert(std::make_pair("CuB_0_LNP",std::cref(CuB_0_LNP)));
63 ModelParamMap.insert(std::make_pair("CuB_u_LNP",std::cref(CuB_u_LNP)));
64 ModelParamMap.insert(std::make_pair("CuB_d_LNP",std::cref(CuB_d_LNP)));
65 ModelParamMap.insert(std::make_pair("CdH_0_LNP",std::cref(CdH_0_LNP)));
66 ModelParamMap.insert(std::make_pair("CdH_u_LNP",std::cref(CdH_u_LNP)));
67 ModelParamMap.insert(std::make_pair("CdH_d_LNP",std::cref(CdH_d_LNP)));
68 ModelParamMap.insert(std::make_pair("CdG_0_LNP",std::cref(CdG_0_LNP)));
69 ModelParamMap.insert(std::make_pair("CdG_u_LNP",std::cref(CdG_u_LNP)));
70 ModelParamMap.insert(std::make_pair("CdG_d_LNP",std::cref(CdG_d_LNP)));
71 ModelParamMap.insert(std::make_pair("CdW_0_LNP",std::cref(CdW_0_LNP)));
72 ModelParamMap.insert(std::make_pair("CdW_u_LNP",std::cref(CdW_u_LNP)));
73 ModelParamMap.insert(std::make_pair("CdW_d_LNP",std::cref(CdW_d_LNP)));
74 ModelParamMap.insert(std::make_pair("CdB_0_LNP",std::cref(CdB_0_LNP)));
75 ModelParamMap.insert(std::make_pair("CdB_u_LNP",std::cref(CdB_u_LNP)));
76 ModelParamMap.insert(std::make_pair("CdB_d_LNP",std::cref(CdB_d_LNP)));
77 ModelParamMap.insert(std::make_pair("CHq1_0_LNP",std::cref(CHq1_0_LNP)));
78 ModelParamMap.insert(std::make_pair("CHq1_u_LNP",std::cref(CHq1_u_LNP)));
79 ModelParamMap.insert(std::make_pair("CHq1_d_LNP",std::cref(CHq1_d_LNP)));
80 ModelParamMap.insert(std::make_pair("CHq3_0_LNP",std::cref(CHq3_0_LNP)));
81 ModelParamMap.insert(std::make_pair("CHq3_u_LNP",std::cref(CHq3_u_LNP)));
82 ModelParamMap.insert(std::make_pair("CHq3_d_LNP",std::cref(CHq3_d_LNP)));
83 ModelParamMap.insert(std::make_pair("CHu_0_LNP",std::cref(CHu_0_LNP)));
84 ModelParamMap.insert(std::make_pair("CHu_u_LNP",std::cref(CHu_u_LNP)));
85 ModelParamMap.insert(std::make_pair("CHd_0_LNP",std::cref(CHd_0_LNP)));
86 ModelParamMap.insert(std::make_pair("CHd_d_LNP",std::cref(CHd_d_LNP)));
87 ModelParamMap.insert(std::make_pair("CHud_ud_LNP",std::cref(CHud_ud_LNP)));
88 ModelParamMap.insert(std::make_pair("Clq1_0_LNP",std::cref(Clq1_0_LNP)));
89 ModelParamMap.insert(std::make_pair("Clq1_u_LNP",std::cref(Clq1_u_LNP)));
90 ModelParamMap.insert(std::make_pair("Clq1_d_LNP",std::cref(Clq1_d_LNP)));
91 ModelParamMap.insert(std::make_pair("Clq3_0_LNP",std::cref(Clq3_0_LNP)));
92 ModelParamMap.insert(std::make_pair("Clq3_u_LNP",std::cref(Clq3_u_LNP)));
93 ModelParamMap.insert(std::make_pair("Clq3_d_LNP",std::cref(Clq3_d_LNP)));
94 ModelParamMap.insert(std::make_pair("Cqe_0_LNP",std::cref(Cqe_0_LNP)));
95 ModelParamMap.insert(std::make_pair("Cqe_u_LNP",std::cref(Cqe_u_LNP)));
96 ModelParamMap.insert(std::make_pair("Cqe_d_LNP",std::cref(Cqe_d_LNP)));
97 ModelParamMap.insert(std::make_pair("Clu_0_LNP",std::cref(Clu_0_LNP)));
98 ModelParamMap.insert(std::make_pair("Clu_u_LNP",std::cref(Clu_u_LNP)));
99 ModelParamMap.insert(std::make_pair("Ceu_0_LNP",std::cref(Ceu_0_LNP)));
100 ModelParamMap.insert(std::make_pair("Ceu_u_LNP",std::cref(Ceu_u_LNP)));
101 ModelParamMap.insert(std::make_pair("Cld_0_LNP",std::cref(Cld_0_LNP)));
102 ModelParamMap.insert(std::make_pair("Cld_d_LNP",std::cref(Cld_d_LNP)));
103 ModelParamMap.insert(std::make_pair("Ced_0_LNP",std::cref(Ced_0_LNP)));
104 ModelParamMap.insert(std::make_pair("Ced_d_LNP",std::cref(Ced_d_LNP)));
105 ModelParamMap.insert(std::make_pair("Cqq1_00_LNP",std::cref(Cqq1_00_LNP)));
106 ModelParamMap.insert(std::make_pair("Cqq1_0u_LNP",std::cref(Cqq1_0u_LNP)));
107 ModelParamMap.insert(std::make_pair("Cqq1_0d_LNP",std::cref(Cqq1_0d_LNP)));
108 ModelParamMap.insert(std::make_pair("Cqq1_u0_LNP",std::cref(Cqq1_u0_LNP)));
109 ModelParamMap.insert(std::make_pair("Cqq1_uu_LNP",std::cref(Cqq1_uu_LNP)));
110 ModelParamMap.insert(std::make_pair("Cqq1_ud_LNP",std::cref(Cqq1_ud_LNP)));
111 ModelParamMap.insert(std::make_pair("Cqq1_d0_LNP",std::cref(Cqq1_d0_LNP)));
112 ModelParamMap.insert(std::make_pair("Cqq1_du_LNP",std::cref(Cqq1_du_LNP)));
113 ModelParamMap.insert(std::make_pair("Cqq1_dd_LNP",std::cref(Cqq1_dd_LNP)));
114 ModelParamMap.insert(std::make_pair("Cqq3_00_LNP",std::cref(Cqq3_00_LNP)));
115 ModelParamMap.insert(std::make_pair("Cqq3_0u_LNP",std::cref(Cqq3_0u_LNP)));
116 ModelParamMap.insert(std::make_pair("Cqq3_0d_LNP",std::cref(Cqq3_0d_LNP)));
117 ModelParamMap.insert(std::make_pair("Cqq3_u0_LNP",std::cref(Cqq3_u0_LNP)));
118 ModelParamMap.insert(std::make_pair("Cqq3_uu_LNP",std::cref(Cqq3_uu_LNP)));
119 ModelParamMap.insert(std::make_pair("Cqq3_ud_LNP",std::cref(Cqq3_ud_LNP)));
120 ModelParamMap.insert(std::make_pair("Cqq3_d0_LNP",std::cref(Cqq3_d0_LNP)));
121 ModelParamMap.insert(std::make_pair("Cqq3_du_LNP",std::cref(Cqq3_du_LNP)));
122 ModelParamMap.insert(std::make_pair("Cqq3_dd_LNP",std::cref(Cqq3_dd_LNP)));
123 ModelParamMap.insert(std::make_pair("Cuu_00_LNP",std::cref(Cuu_00_LNP)));
124 ModelParamMap.insert(std::make_pair("Cuu_0u_LNP",std::cref(Cuu_0u_LNP)));
125 ModelParamMap.insert(std::make_pair("Cuu_u0_LNP",std::cref(Cuu_u0_LNP)));
126 ModelParamMap.insert(std::make_pair("Cuu_uu_LNP",std::cref(Cuu_uu_LNP)));
127 ModelParamMap.insert(std::make_pair("Cdd_00_LNP",std::cref(Cdd_00_LNP)));
128 ModelParamMap.insert(std::make_pair("Cdd_0d_LNP",std::cref(Cdd_0d_LNP)));
129 ModelParamMap.insert(std::make_pair("Cdd_d0_LNP",std::cref(Cdd_d0_LNP)));
130 ModelParamMap.insert(std::make_pair("Cdd_dd_LNP",std::cref(Cdd_dd_LNP)));
131 ModelParamMap.insert(std::make_pair("Cud1_00_LNP",std::cref(Cud1_00_LNP)));
132 ModelParamMap.insert(std::make_pair("Cud1_u0_LNP",std::cref(Cud1_u0_LNP)));
133 ModelParamMap.insert(std::make_pair("Cud1_0d_LNP",std::cref(Cud1_0d_LNP)));
134 ModelParamMap.insert(std::make_pair("Cud1_ud_LNP",std::cref(Cud1_ud_LNP)));
135 ModelParamMap.insert(std::make_pair("Cud8_00_LNP",std::cref(Cud8_00_LNP)));
136 ModelParamMap.insert(std::make_pair("Cud8_u0_LNP",std::cref(Cud8_u0_LNP)));
137 ModelParamMap.insert(std::make_pair("Cud8_0d_LNP",std::cref(Cud8_0d_LNP)));
138 ModelParamMap.insert(std::make_pair("Cud8_ud_LNP",std::cref(Cud8_ud_LNP)));
139 ModelParamMap.insert(std::make_pair("Cqu1_00_LNP",std::cref(Cqu1_00_LNP)));
140 ModelParamMap.insert(std::make_pair("Cqu1_u0_LNP",std::cref(Cqu1_u0_LNP)));
141 ModelParamMap.insert(std::make_pair("Cqu1_d0_LNP",std::cref(Cqu1_d0_LNP)));
142 ModelParamMap.insert(std::make_pair("Cqu1_0u_LNP",std::cref(Cqu1_0u_LNP)));
143 ModelParamMap.insert(std::make_pair("Cqu1_uu_LNP",std::cref(Cqu1_uu_LNP)));
144 ModelParamMap.insert(std::make_pair("Cqu1_du_LNP",std::cref(Cqu1_du_LNP)));
145 ModelParamMap.insert(std::make_pair("Cqu8_00_LNP",std::cref(Cqu8_00_LNP)));
146 ModelParamMap.insert(std::make_pair("Cqu8_u0_LNP",std::cref(Cqu8_u0_LNP)));
147 ModelParamMap.insert(std::make_pair("Cqu8_d0_LNP",std::cref(Cqu8_d0_LNP)));
148 ModelParamMap.insert(std::make_pair("Cqu8_0u_LNP",std::cref(Cqu8_0u_LNP)));
149 ModelParamMap.insert(std::make_pair("Cqu8_uu_LNP",std::cref(Cqu8_uu_LNP)));
150 ModelParamMap.insert(std::make_pair("Cqu8_du_LNP",std::cref(Cqu8_du_LNP)));
151 ModelParamMap.insert(std::make_pair("Cqd1_00_LNP",std::cref(Cqd1_00_LNP)));
152 ModelParamMap.insert(std::make_pair("Cqd1_u0_LNP",std::cref(Cqd1_u0_LNP)));
153 ModelParamMap.insert(std::make_pair("Cqd1_d0_LNP",std::cref(Cqd1_d0_LNP)));
154 ModelParamMap.insert(std::make_pair("Cqd1_0d_LNP",std::cref(Cqd1_0d_LNP)));
155 ModelParamMap.insert(std::make_pair("Cqd1_ud_LNP",std::cref(Cqd1_ud_LNP)));
156 ModelParamMap.insert(std::make_pair("Cqd1_dd_LNP",std::cref(Cqd1_dd_LNP)));
157 ModelParamMap.insert(std::make_pair("Cqd8_00_LNP",std::cref(Cqd8_00_LNP)));
158 ModelParamMap.insert(std::make_pair("Cqd8_u0_LNP",std::cref(Cqd8_u0_LNP)));
159 ModelParamMap.insert(std::make_pair("Cqd8_d0_LNP",std::cref(Cqd8_d0_LNP)));
160 ModelParamMap.insert(std::make_pair("Cqd8_0d_LNP",std::cref(Cqd8_0d_LNP)));
161 ModelParamMap.insert(std::make_pair("Cqd8_ud_LNP",std::cref(Cqd8_ud_LNP)));
162 ModelParamMap.insert(std::make_pair("Cqd8_dd_LNP",std::cref(Cqd8_dd_LNP)));
163 ModelParamMap.insert(std::make_pair("Cquqd1_00_LNP",std::cref(Cquqd1_00_LNP)));
164 ModelParamMap.insert(std::make_pair("Cquqd8_00_LNP",std::cref(Cquqd8_00_LNP)));
165
166}
std::map< std::string, std::reference_wrapper< const double > > ModelParamMap
Definition: Model.h:280
void setModelName(const std::string name)
A method to set the name of the model.
Definition: Model.h:50
double CW_LNP
The dimension-6 operator coefficient .
double CHbox_LNP
The dimension-6 operator coefficient .
NPSMEFTd6General()
Constructor.
double CHG_LNP
The dimension-6 operator coefficient .
double CHD_LNP
The dimension-6 operator coefficient .
double CHB_LNP
The dimension-6 operator coefficient .
double CHWB_LNP
The dimension-6 operator coefficient .
double CG_LNP
The dimension-6 operator coefficient .
double CHW_LNP
The dimension-6 operator coefficient .
double CH_LNP
The dimension-6 operator coefficient .
double Cqq3_00_LNP
Definition: NPSMEFTd6MFV.h:127
double Cuu_0u_LNP
Definition: NPSMEFTd6MFV.h:130
double CuH_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:64
double Clq1_u_LNP
Definition: NPSMEFTd6MFV.h:103
double Cqe_u_LNP
Definition: NPSMEFTd6MFV.h:109
double CHq3_0_LNP
Definition: NPSMEFTd6MFV.h:91
double Cud1_u0_LNP
Definition: NPSMEFTd6MFV.h:136
double Ced_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:121
double Cqd1_u0_LNP
Definition: NPSMEFTd6MFV.h:148
double Cqq1_ud_LNP
Definition: NPSMEFTd6MFV.h:124
double Cquqd1_00_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:154
double Cqq3_dd_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:127
double Cud8_u0_LNP
Definition: NPSMEFTd6MFV.h:139
double Cqd8_d0_LNP
Definition: NPSMEFTd6MFV.h:151
double CdB_u_LNP
Definition: NPSMEFTd6MFV.h:85
double Cqq1_0u_LNP
Definition: NPSMEFTd6MFV.h:124
double Cud8_0d_LNP
Definition: NPSMEFTd6MFV.h:139
double Cqq3_ud_LNP
Definition: NPSMEFTd6MFV.h:127
double Clq3_u_LNP
Definition: NPSMEFTd6MFV.h:106
double Cquqd8_00_LNP
Definition: NPSMEFTd6MFV.h:157
double CHu_0_LNP
Definition: NPSMEFTd6MFV.h:94
double Ceu_u_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:115
double CHe_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:49
double Cqd1_d0_LNP
Definition: NPSMEFTd6MFV.h:148
double CuB_u_LNP
Definition: NPSMEFTd6MFV.h:73
double CHd_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:97
double Clq3_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:106
double CdG_u_LNP
Definition: NPSMEFTd6MFV.h:79
double CuG_u_LNP
Definition: NPSMEFTd6MFV.h:67
double CuW_0_LNP
Definition: NPSMEFTd6MFV.h:70
double CdH_u_LNP
Definition: NPSMEFTd6MFV.h:76
double CdW_u_LNP
Definition: NPSMEFTd6MFV.h:82
double Cqu1_du_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:142
double CHl3_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:46
double CHd_0_LNP
Definition: NPSMEFTd6MFV.h:97
double CdG_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:79
double CuW_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:70
double Ced_0_LNP
Definition: NPSMEFTd6MFV.h:121
double Clq3_0_LNP
Definition: NPSMEFTd6MFV.h:106
double Cqu1_u0_LNP
Definition: NPSMEFTd6MFV.h:142
double Cqq3_u0_LNP
Definition: NPSMEFTd6MFV.h:127
double Clq1_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:103
double Cll_abba_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:55
double CuG_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:67
double Cee_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:58
double CuW_u_LNP
Definition: NPSMEFTd6MFV.h:70
double Cqq3_0d_LNP
Definition: NPSMEFTd6MFV.h:127
double Cll_aabb_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:52
double Cqu1_0u_LNP
Definition: NPSMEFTd6MFV.h:142
double Cqq1_dd_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:124
double Cqd8_ud_LNP
Definition: NPSMEFTd6MFV.h:151
double Cqu8_0u_LNP
Definition: NPSMEFTd6MFV.h:145
double Cqq3_uu_LNP
Definition: NPSMEFTd6MFV.h:127
double CuB_0_LNP
Definition: NPSMEFTd6MFV.h:73
double Cqq1_d0_LNP
Definition: NPSMEFTd6MFV.h:124
double Cqd8_dd_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:151
double Cqd1_dd_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:148
double Cqq3_du_LNP
Definition: NPSMEFTd6MFV.h:127
double CdH_0_LNP
Definition: NPSMEFTd6MFV.h:76
double Cqu1_00_LNP
Definition: NPSMEFTd6MFV.h:142
double CHu_u_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:94
double Cuu_00_LNP
Definition: NPSMEFTd6MFV.h:130
double Cuu_uu_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:130
double CHq3_u_LNP
Definition: NPSMEFTd6MFV.h:91
double Cqq1_0d_LNP
Definition: NPSMEFTd6MFV.h:124
double Cdd_dd_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:133
double Cqu1_d0_LNP
Definition: NPSMEFTd6MFV.h:142
double CHq1_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:88
double CdB_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:85
double Cdd_0d_LNP
Definition: NPSMEFTd6MFV.h:133
double CHud_ud_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:100
double CdB_0_LNP
Definition: NPSMEFTd6MFV.h:85
double CHq1_0_LNP
Definition: NPSMEFTd6MFV.h:88
double CdH_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:76
double Cqd8_u0_LNP
Definition: NPSMEFTd6MFV.h:151
double Cud1_ud_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:136
double CdG_0_LNP
Definition: NPSMEFTd6MFV.h:79
double Cqq1_00_LNP
Definition: NPSMEFTd6MFV.h:124
double CuH_u_LNP
Definition: NPSMEFTd6MFV.h:64
double Ceu_0_LNP
Definition: NPSMEFTd6MFV.h:115
double Clq1_0_LNP
Definition: NPSMEFTd6MFV.h:103
double Cdd_00_LNP
Definition: NPSMEFTd6MFV.h:133
double Cqq1_du_LNP
Definition: NPSMEFTd6MFV.h:124
double Clu_0_LNP
Definition: NPSMEFTd6MFV.h:112
double Cqq1_uu_LNP
Definition: NPSMEFTd6MFV.h:124
double Cud8_00_LNP
Definition: NPSMEFTd6MFV.h:139
double Clu_u_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:112
double Cqq3_d0_LNP
Definition: NPSMEFTd6MFV.h:127
double CuH_0_LNP
Definition: NPSMEFTd6MFV.h:64
double Cuu_u0_LNP
Definition: NPSMEFTd6MFV.h:130
double Cqd8_0d_LNP
Definition: NPSMEFTd6MFV.h:151
double Cqq1_u0_LNP
Definition: NPSMEFTd6MFV.h:124
double Cqu8_d0_LNP
Definition: NPSMEFTd6MFV.h:145
double CHq1_u_LNP
Definition: NPSMEFTd6MFV.h:88
double Cud8_ud_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:139
double Cqu8_uu_LNP
Definition: NPSMEFTd6MFV.h:145
double Cqu8_du_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:145
double Cqe_0_LNP
Definition: NPSMEFTd6MFV.h:109
double CdW_0_LNP
Definition: NPSMEFTd6MFV.h:82
double Cqd1_00_LNP
Definition: NPSMEFTd6MFV.h:148
double CHl1_LNP
< Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:43
double Cqq3_0u_LNP
Definition: NPSMEFTd6MFV.h:127
double Cld_0_LNP
Definition: NPSMEFTd6MFV.h:118
double Cld_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:118
double Cud1_0d_LNP
Definition: NPSMEFTd6MFV.h:136
double CuB_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:73
double Cqd1_0d_LNP
Definition: NPSMEFTd6MFV.h:148
double Cqu8_00_LNP
Definition: NPSMEFTd6MFV.h:145
double Cqd1_ud_LNP
Definition: NPSMEFTd6MFV.h:148
double Cud1_00_LNP
Definition: NPSMEFTd6MFV.h:136
double CuG_0_LNP
Definition: NPSMEFTd6MFV.h:67
double Cdd_d0_LNP
Definition: NPSMEFTd6MFV.h:133
double Cqu8_u0_LNP
Definition: NPSMEFTd6MFV.h:145
double Cle_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:61
double Cqd8_00_LNP
Definition: NPSMEFTd6MFV.h:151
double Cqu1_uu_LNP
Definition: NPSMEFTd6MFV.h:142
double CdW_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:82
double Cqe_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:109
double CHq3_d_LNP
Coefficients of the MFV expansion of the dimension-6 operator coefficient .
Definition: NPSMEFTd6MFV.h:91

Member Function Documentation

◆ Init()

bool NPSMEFTd6MFV::Init ( const std::map< std::string, double > &  DPars)
virtual

A method to initialize the model parameters.

Parameters
[in]DParsa map of the parameters that are being updated in the Monte Carlo run (including parameters that are varied and those that are held constant)
Returns
a boolean that is true if the execution is successful

Reimplemented from NPSMEFTd6General.

Definition at line 168 of file NPSMEFTd6MFV.cpp.

168 {
169 if (SMEFTBasisFlag == "UP")
170 throw std::runtime_error("Bad argument in SMEFTBasisFlag. (Only DOWN is allowed for this Model)");
171
173}
std::map< std::string, double > DPars
Definition: Minimal.cpp:11
virtual bool Init(const std::map< std::string, double > &DPars)
A method to initialize the model parameters.
std::string SMEFTBasisFlag

◆ PostUpdate()

bool NPSMEFTd6MFV::PostUpdate ( )
virtual

The post-update method for NPSMEFTd6General.

This method runs all the procedures that are need to be executed after the model is successfully updated.

Returns
a boolean that is true if the execution is successful

Reimplemented from NPSMEFTd6General.

Definition at line 1469 of file NPSMEFTd6MFV.cpp.

1469 {
1470
1472
1474
1475 if (!NPSMEFTd6General::PostUpdate()) return (false);
1476
1477 return (true);
1478}
virtual bool PostUpdate()
The post-update method for NPSMEFTd6General.
void GenerateSMInitialConditions()
Generates the initial condition for the Standard Model parameters.
void setNPSMEFTd6GeneralParameters()
An auxiliary method to set the WC of the general class.

◆ setNPSMEFTd6GeneralParameters()

void NPSMEFTd6MFV::setNPSMEFTd6GeneralParameters ( )
protected

An auxiliary method to set the WC of the general class.

Definition at line 439 of file NPSMEFTd6MFV.cpp.

439 {
440 gslpp::vector<gslpp::complex> YdL(3, 0.), YddL(3, 0.), YdddL(3, 0.);
441 gslpp::matrix<gslpp::complex> YuL(3, 3, 0.), YdML(3, 3, 0.);
442 gslpp::matrix<gslpp::complex> YucuL(3, 3, 0.), YuucL(3, 3, 0.), YudL(3, 3, 0.);
443 gslpp::matrix<gslpp::complex> YucuuL(3, 3, 0.), YdduL(3, 3, 0.), YucudL(3, 3, 0.);
444
445 // Create the up-Yukawa matrix
446 for (int i = 0; i < 3; i++) {
447 for (int j = 0; j < 3; j++) {
448 YuL.assignre(i, j, getSMEFTCoeffEW("YuR", i, j));
449 YuL.assignim(i, j, getSMEFTCoeffEW("YuI", i, j));
450 }
451 }
452
453 // Create the down-Yukawa diagonal matrix and its powers
454 for (int i = 0; i < 3; i++) {
455 double ydi = getSMEFTCoeffEW("YdR", i, i);
456 YdML.assign(i, i, ydi);
457 YdL.assign(i, ydi);
458 YddL.assign(i, ydi*ydi);
459 YdddL.assign(i, ydi*ydi*ydi);
460 }
461
462 // Products of two Yukawas
463 YucuL = YuL.hconjugate() * YuL;
464 YuucL = YuL * YuL.hconjugate();
465 YudL = YuL * YdML;
466
467 // Products of three Yukawas
468 YucuuL = YucuL * YuL;
469 YdduL = YdML * YdML * YuL;
470 YucudL = YucuL * YdML;
471
472 // Operator assignments
473
477
481
485
495
496 CuH_11r_LNP = (CuH_d_LNP*YdduL(0,0) + CuH_u_LNP*YucuuL(0,0) + CuH_0_LNP*YuL(0,0)).real();
497 CuH_11i_LNP = (CuH_d_LNP*YdduL(0,0) + CuH_u_LNP*YucuuL(0,0) + CuH_0_LNP*YuL(0,0)).imag();
498 CuH_12r_LNP = (CuH_d_LNP*YdduL(0,1) + CuH_u_LNP*YucuuL(0,1) + CuH_0_LNP*YuL(0,1)).real();
499 CuH_12i_LNP = (CuH_d_LNP*YdduL(0,1) + CuH_u_LNP*YucuuL(0,1) + CuH_0_LNP*YuL(0,1)).imag();
500 CuH_13r_LNP = (CuH_d_LNP*YdduL(0,2) + CuH_u_LNP*YucuuL(0,2) + CuH_0_LNP*YuL(0,2)).real();
501 CuH_13i_LNP = (CuH_d_LNP*YdduL(0,2) + CuH_u_LNP*YucuuL(0,2) + CuH_0_LNP*YuL(0,2)).imag();
502 CuH_21r_LNP = (CuH_d_LNP*YdduL(1,0) + CuH_u_LNP*YucuuL(1,0) + CuH_0_LNP*YuL(1,0)).real();
503 CuH_21i_LNP = (CuH_d_LNP*YdduL(1,0) + CuH_u_LNP*YucuuL(1,0) + CuH_0_LNP*YuL(1,0)).imag();
504 CuH_22r_LNP = (CuH_d_LNP*YdduL(1,1) + CuH_u_LNP*YucuuL(1,1) + CuH_0_LNP*YuL(1,1)).real();
505 CuH_22i_LNP = (CuH_d_LNP*YdduL(1,1) + CuH_u_LNP*YucuuL(1,1) + CuH_0_LNP*YuL(1,1)).imag();
506 CuH_23r_LNP = (CuH_d_LNP*YdduL(1,2) + CuH_u_LNP*YucuuL(1,2) + CuH_0_LNP*YuL(1,2)).real();
507 CuH_23i_LNP = (CuH_d_LNP*YdduL(1,2) + CuH_u_LNP*YucuuL(1,2) + CuH_0_LNP*YuL(1,2)).imag();
508 CuH_31r_LNP = (CuH_d_LNP*YdduL(2,0) + CuH_u_LNP*YucuuL(2,0) + CuH_0_LNP*YuL(2,0)).real();
509 CuH_31i_LNP = (CuH_d_LNP*YdduL(2,0) + CuH_u_LNP*YucuuL(2,0) + CuH_0_LNP*YuL(2,0)).imag();
510 CuH_32r_LNP = (CuH_d_LNP*YdduL(2,1) + CuH_u_LNP*YucuuL(2,1) + CuH_0_LNP*YuL(2,1)).real();
511 CuH_32i_LNP = (CuH_d_LNP*YdduL(2,1) + CuH_u_LNP*YucuuL(2,1) + CuH_0_LNP*YuL(2,1)).imag();
512 CuH_33r_LNP = (CuH_d_LNP*YdduL(2,2) + CuH_u_LNP*YucuuL(2,2) + CuH_0_LNP*YuL(2,2)).real();
513 CuH_33i_LNP = (CuH_d_LNP*YdduL(2,2) + CuH_u_LNP*YucuuL(2,2) + CuH_0_LNP*YuL(2,2)).imag();
514
515 CuG_11r_LNP = (CuG_d_LNP*YdduL(0,0) + CuG_u_LNP*YucuuL(0,0) + CuG_0_LNP*YuL(0,0)).real();
516 CuG_11i_LNP = (CuG_d_LNP*YdduL(0,0) + CuG_u_LNP*YucuuL(0,0) + CuG_0_LNP*YuL(0,0)).imag();
517 CuG_12r_LNP = (CuG_d_LNP*YdduL(0,1) + CuG_u_LNP*YucuuL(0,1) + CuG_0_LNP*YuL(0,1)).real();
518 CuG_12i_LNP = (CuG_d_LNP*YdduL(0,1) + CuG_u_LNP*YucuuL(0,1) + CuG_0_LNP*YuL(0,1)).imag();
519 CuG_13r_LNP = (CuG_d_LNP*YdduL(0,2) + CuG_u_LNP*YucuuL(0,2) + CuG_0_LNP*YuL(0,2)).real();
520 CuG_13i_LNP = (CuG_d_LNP*YdduL(0,2) + CuG_u_LNP*YucuuL(0,2) + CuG_0_LNP*YuL(0,2)).imag();
521 CuG_21r_LNP = (CuG_d_LNP*YdduL(1,0) + CuG_u_LNP*YucuuL(1,0) + CuG_0_LNP*YuL(1,0)).real();
522 CuG_21i_LNP = (CuG_d_LNP*YdduL(1,0) + CuG_u_LNP*YucuuL(1,0) + CuG_0_LNP*YuL(1,0)).imag();
523 CuG_22r_LNP = (CuG_d_LNP*YdduL(1,1) + CuG_u_LNP*YucuuL(1,1) + CuG_0_LNP*YuL(1,1)).real();
524 CuG_22i_LNP = (CuG_d_LNP*YdduL(1,1) + CuG_u_LNP*YucuuL(1,1) + CuG_0_LNP*YuL(1,1)).imag();
525 CuG_23r_LNP = (CuG_d_LNP*YdduL(1,2) + CuG_u_LNP*YucuuL(1,2) + CuG_0_LNP*YuL(1,2)).real();
526 CuG_23i_LNP = (CuG_d_LNP*YdduL(1,2) + CuG_u_LNP*YucuuL(1,2) + CuG_0_LNP*YuL(1,2)).imag();
527 CuG_31r_LNP = (CuG_d_LNP*YdduL(2,0) + CuG_u_LNP*YucuuL(2,0) + CuG_0_LNP*YuL(2,0)).real();
528 CuG_31i_LNP = (CuG_d_LNP*YdduL(2,0) + CuG_u_LNP*YucuuL(2,0) + CuG_0_LNP*YuL(2,0)).imag();
529 CuG_32r_LNP = (CuG_d_LNP*YdduL(2,1) + CuG_u_LNP*YucuuL(2,1) + CuG_0_LNP*YuL(2,1)).real();
530 CuG_32i_LNP = (CuG_d_LNP*YdduL(2,1) + CuG_u_LNP*YucuuL(2,1) + CuG_0_LNP*YuL(2,1)).imag();
531 CuG_33r_LNP = (CuG_d_LNP*YdduL(2,2) + CuG_u_LNP*YucuuL(2,2) + CuG_0_LNP*YuL(2,2)).real();
532 CuG_33i_LNP = (CuG_d_LNP*YdduL(2,2) + CuG_u_LNP*YucuuL(2,2) + CuG_0_LNP*YuL(2,2)).imag();
533
534 CuW_11r_LNP = (CuW_d_LNP*YdduL(0,0) + CuW_u_LNP*YucuuL(0,0) + CuW_0_LNP*YuL(0,0)).real();
535 CuW_11i_LNP = (CuW_d_LNP*YdduL(0,0) + CuW_u_LNP*YucuuL(0,0) + CuW_0_LNP*YuL(0,0)).imag();
536 CuW_12r_LNP = (CuW_d_LNP*YdduL(0,1) + CuW_u_LNP*YucuuL(0,1) + CuW_0_LNP*YuL(0,1)).real();
537 CuW_12i_LNP = (CuW_d_LNP*YdduL(0,1) + CuW_u_LNP*YucuuL(0,1) + CuW_0_LNP*YuL(0,1)).imag();
538 CuW_13r_LNP = (CuW_d_LNP*YdduL(0,2) + CuW_u_LNP*YucuuL(0,2) + CuW_0_LNP*YuL(0,2)).real();
539 CuW_13i_LNP = (CuW_d_LNP*YdduL(0,2) + CuW_u_LNP*YucuuL(0,2) + CuW_0_LNP*YuL(0,2)).imag();
540 CuW_21r_LNP = (CuW_d_LNP*YdduL(1,0) + CuW_u_LNP*YucuuL(1,0) + CuW_0_LNP*YuL(1,0)).real();
541 CuW_21i_LNP = (CuW_d_LNP*YdduL(1,0) + CuW_u_LNP*YucuuL(1,0) + CuW_0_LNP*YuL(1,0)).imag();
542 CuW_22r_LNP = (CuW_d_LNP*YdduL(1,1) + CuW_u_LNP*YucuuL(1,1) + CuW_0_LNP*YuL(1,1)).real();
543 CuW_22i_LNP = (CuW_d_LNP*YdduL(1,1) + CuW_u_LNP*YucuuL(1,1) + CuW_0_LNP*YuL(1,1)).imag();
544 CuW_23r_LNP = (CuW_d_LNP*YdduL(1,2) + CuW_u_LNP*YucuuL(1,2) + CuW_0_LNP*YuL(1,2)).real();
545 CuW_23i_LNP = (CuW_d_LNP*YdduL(1,2) + CuW_u_LNP*YucuuL(1,2) + CuW_0_LNP*YuL(1,2)).imag();
546 CuW_31r_LNP = (CuW_d_LNP*YdduL(2,0) + CuW_u_LNP*YucuuL(2,0) + CuW_0_LNP*YuL(2,0)).real();
547 CuW_31i_LNP = (CuW_d_LNP*YdduL(2,0) + CuW_u_LNP*YucuuL(2,0) + CuW_0_LNP*YuL(2,0)).imag();
548 CuW_32r_LNP = (CuW_d_LNP*YdduL(2,1) + CuW_u_LNP*YucuuL(2,1) + CuW_0_LNP*YuL(2,1)).real();
549 CuW_32i_LNP = (CuW_d_LNP*YdduL(2,1) + CuW_u_LNP*YucuuL(2,1) + CuW_0_LNP*YuL(2,1)).imag();
550 CuW_33r_LNP = (CuW_d_LNP*YdduL(2,2) + CuW_u_LNP*YucuuL(2,2) + CuW_0_LNP*YuL(2,2)).real();
551 CuW_33i_LNP = (CuW_d_LNP*YdduL(2,2) + CuW_u_LNP*YucuuL(2,2) + CuW_0_LNP*YuL(2,2)).imag();
552
553 CuB_11r_LNP = (CuB_d_LNP*YdduL(0,0) + CuB_u_LNP*YucuuL(0,0) + CuB_0_LNP*YuL(0,0)).real();
554 CuB_11i_LNP = (CuB_d_LNP*YdduL(0,0) + CuB_u_LNP*YucuuL(0,0) + CuB_0_LNP*YuL(0,0)).imag();
555 CuB_12r_LNP = (CuB_d_LNP*YdduL(0,1) + CuB_u_LNP*YucuuL(0,1) + CuB_0_LNP*YuL(0,1)).real();
556 CuB_12i_LNP = (CuB_d_LNP*YdduL(0,1) + CuB_u_LNP*YucuuL(0,1) + CuB_0_LNP*YuL(0,1)).imag();
557 CuB_13r_LNP = (CuB_d_LNP*YdduL(0,2) + CuB_u_LNP*YucuuL(0,2) + CuB_0_LNP*YuL(0,2)).real();
558 CuB_13i_LNP = (CuB_d_LNP*YdduL(0,2) + CuB_u_LNP*YucuuL(0,2) + CuB_0_LNP*YuL(0,2)).imag();
559 CuB_21r_LNP = (CuB_d_LNP*YdduL(1,0) + CuB_u_LNP*YucuuL(1,0) + CuB_0_LNP*YuL(1,0)).real();
560 CuB_21i_LNP = (CuB_d_LNP*YdduL(1,0) + CuB_u_LNP*YucuuL(1,0) + CuB_0_LNP*YuL(1,0)).imag();
561 CuB_22r_LNP = (CuB_d_LNP*YdduL(1,1) + CuB_u_LNP*YucuuL(1,1) + CuB_0_LNP*YuL(1,1)).real();
562 CuB_22i_LNP = (CuB_d_LNP*YdduL(1,1) + CuB_u_LNP*YucuuL(1,1) + CuB_0_LNP*YuL(1,1)).imag();
563 CuB_23r_LNP = (CuB_d_LNP*YdduL(1,2) + CuB_u_LNP*YucuuL(1,2) + CuB_0_LNP*YuL(1,2)).real();
564 CuB_23i_LNP = (CuB_d_LNP*YdduL(1,2) + CuB_u_LNP*YucuuL(1,2) + CuB_0_LNP*YuL(1,2)).imag();
565 CuB_31r_LNP = (CuB_d_LNP*YdduL(2,0) + CuB_u_LNP*YucuuL(2,0) + CuB_0_LNP*YuL(2,0)).real();
566 CuB_31i_LNP = (CuB_d_LNP*YdduL(2,0) + CuB_u_LNP*YucuuL(2,0) + CuB_0_LNP*YuL(2,0)).imag();
567 CuB_32r_LNP = (CuB_d_LNP*YdduL(2,1) + CuB_u_LNP*YucuuL(2,1) + CuB_0_LNP*YuL(2,1)).real();
568 CuB_32i_LNP = (CuB_d_LNP*YdduL(2,1) + CuB_u_LNP*YucuuL(2,1) + CuB_0_LNP*YuL(2,1)).imag();
569 CuB_33r_LNP = (CuB_d_LNP*YdduL(2,2) + CuB_u_LNP*YucuuL(2,2) + CuB_0_LNP*YuL(2,2)).real();
570 CuB_33i_LNP = (CuB_d_LNP*YdduL(2,2) + CuB_u_LNP*YucuuL(2,2) + CuB_0_LNP*YuL(2,2)).imag();
571
572 CdH_11r_LNP = (CdH_d_LNP*YdddL(0) + CdH_0_LNP*YdL(0) + CdH_u_LNP*YucudL(0,0)).real();
573 CdH_11i_LNP = (CdH_d_LNP*YdddL(0) + CdH_0_LNP*YdL(0) + CdH_u_LNP*YucudL(0,0)).imag();
574 CdH_12r_LNP = (CdH_u_LNP*YucudL(0,1)).real();
575 CdH_12i_LNP = (CdH_u_LNP*YucudL(0,1)).imag();
576 CdH_13r_LNP = (CdH_u_LNP*YucudL(0,2)).real();
577 CdH_13i_LNP = (CdH_u_LNP*YucudL(0,2)).imag();
578 CdH_21r_LNP = (CdH_u_LNP*YucudL(1,0)).real();
579 CdH_21i_LNP = (CdH_u_LNP*YucudL(1,0)).imag();
580 CdH_22r_LNP = (CdH_d_LNP*YdddL(1) + CdH_0_LNP*YdL(1) + CdH_u_LNP*YucudL(1,1)).real();
581 CdH_22i_LNP = (CdH_d_LNP*YdddL(1) + CdH_0_LNP*YdL(1) + CdH_u_LNP*YucudL(1,1)).imag();
582 CdH_23r_LNP = (CdH_u_LNP*YucudL(1,2)).real();
583 CdH_23i_LNP = (CdH_u_LNP*YucudL(1,2)).imag();
584 CdH_31r_LNP = (CdH_u_LNP*YucudL(2,0)).real();
585 CdH_31i_LNP = (CdH_u_LNP*YucudL(2,0)).imag();
586 CdH_32r_LNP = (CdH_u_LNP*YucudL(2,1)).real();
587 CdH_32i_LNP = (CdH_u_LNP*YucudL(2,1)).imag();
588 CdH_33r_LNP = (CdH_d_LNP*YdddL(2) + CdH_0_LNP*YdL(2) + CdH_u_LNP*YucudL(2,2)).real();
589 CdH_33i_LNP = (CdH_d_LNP*YdddL(2) + CdH_0_LNP*YdL(2) + CdH_u_LNP*YucudL(2,2)).imag();
590
591 CdG_11r_LNP = (CdG_d_LNP*YdddL(0) + CdG_0_LNP*YdL(0) + CdG_u_LNP*YucudL(0,0)).real();
592 CdG_11i_LNP = (CdG_d_LNP*YdddL(0) + CdG_0_LNP*YdL(0) + CdG_u_LNP*YucudL(0,0)).imag();
593 CdG_12r_LNP = (CdG_u_LNP*YucudL(0,1)).real();
594 CdG_12i_LNP = (CdG_u_LNP*YucudL(0,1)).imag();
595 CdG_13r_LNP = (CdG_u_LNP*YucudL(0,2)).real();
596 CdG_13i_LNP = (CdG_u_LNP*YucudL(0,2)).imag();
597 CdG_21r_LNP = (CdG_u_LNP*YucudL(1,0)).real();
598 CdG_21i_LNP = (CdG_u_LNP*YucudL(1,0)).imag();
599 CdG_22r_LNP = (CdG_d_LNP*YdddL(1) + CdG_0_LNP*YdL(1) + CdG_u_LNP*YucudL(1,1)).real();
600 CdG_22i_LNP = (CdG_d_LNP*YdddL(1) + CdG_0_LNP*YdL(1) + CdG_u_LNP*YucudL(1,1)).imag();
601 CdG_23r_LNP = (CdG_u_LNP*YucudL(1,2)).real();
602 CdG_23i_LNP = (CdG_u_LNP*YucudL(1,2)).imag();
603 CdG_31r_LNP = (CdG_u_LNP*YucudL(2,0)).real();
604 CdG_31i_LNP = (CdG_u_LNP*YucudL(2,0)).imag();
605 CdG_32r_LNP = (CdG_u_LNP*YucudL(2,1)).real();
606 CdG_32i_LNP = (CdG_u_LNP*YucudL(2,1)).imag();
607 CdG_33r_LNP = (CdG_d_LNP*YdddL(2) + CdG_0_LNP*YdL(2) + CdG_u_LNP*YucudL(2,2)).real();
608 CdG_33i_LNP = (CdG_d_LNP*YdddL(2) + CdG_0_LNP*YdL(2) + CdG_u_LNP*YucudL(2,2)).imag();
609
610 CdW_11r_LNP = (CdW_d_LNP*YdddL(0) + CdW_0_LNP*YdL(0) + CdW_u_LNP*YucudL(0,0)).real();
611 CdW_11i_LNP = (CdW_d_LNP*YdddL(0) + CdW_0_LNP*YdL(0) + CdW_u_LNP*YucudL(0,0)).imag();
612 CdW_12r_LNP = (CdW_u_LNP*YucudL(0,1)).real();
613 CdW_12i_LNP = (CdW_u_LNP*YucudL(0,1)).imag();
614 CdW_13r_LNP = (CdW_u_LNP*YucudL(0,2)).real();
615 CdW_13i_LNP = (CdW_u_LNP*YucudL(0,2)).imag();
616 CdW_21r_LNP = (CdW_u_LNP*YucudL(1,0)).real();
617 CdW_21i_LNP = (CdW_u_LNP*YucudL(1,0)).imag();
618 CdW_22r_LNP = (CdW_d_LNP*YdddL(1) + CdW_0_LNP*YdL(1) + CdW_u_LNP*YucudL(1,1)).real();
619 CdW_22i_LNP = (CdW_d_LNP*YdddL(1) + CdW_0_LNP*YdL(1) + CdW_u_LNP*YucudL(1,1)).imag();
620 CdW_23r_LNP = (CdW_u_LNP*YucudL(1,2)).real();
621 CdW_23i_LNP = (CdW_u_LNP*YucudL(1,2)).imag();
622 CdW_31r_LNP = (CdW_u_LNP*YucudL(2,0)).real();
623 CdW_31i_LNP = (CdW_u_LNP*YucudL(2,0)).imag();
624 CdW_32r_LNP = (CdW_u_LNP*YucudL(2,1)).real();
625 CdW_32i_LNP = (CdW_u_LNP*YucudL(2,1)).imag();
626 CdW_33r_LNP = (CdW_d_LNP*YdddL(2) + CdW_0_LNP*YdL(2) + CdW_u_LNP*YucudL(2,2)).real();
627 CdW_33i_LNP = (CdW_d_LNP*YdddL(2) + CdW_0_LNP*YdL(2) + CdW_u_LNP*YucudL(2,2)).imag();
628
629 CdB_11r_LNP = (CdB_d_LNP*YdddL(0) + CdB_0_LNP*YdL(0) + CdB_u_LNP*YucudL(0,0)).real();
630 CdB_11i_LNP = (CdB_d_LNP*YdddL(0) + CdB_0_LNP*YdL(0) + CdB_u_LNP*YucudL(0,0)).imag();
631 CdB_12r_LNP = (CdB_u_LNP*YucudL(0,1)).real();
632 CdB_12i_LNP = (CdB_u_LNP*YucudL(0,1)).imag();
633 CdB_13r_LNP = (CdB_u_LNP*YucudL(0,2)).real();
634 CdB_13i_LNP = (CdB_u_LNP*YucudL(0,2)).imag();
635 CdB_21r_LNP = (CdB_u_LNP*YucudL(1,0)).real();
636 CdB_21i_LNP = (CdB_u_LNP*YucudL(1,0)).imag();
637 CdB_22r_LNP = (CdB_d_LNP*YdddL(1) + CdB_0_LNP*YdL(1) + CdB_u_LNP*YucudL(1,1)).real();
638 CdB_22i_LNP = (CdB_d_LNP*YdddL(1) + CdB_0_LNP*YdL(1) + CdB_u_LNP*YucudL(1,1)).imag();
639 CdB_23r_LNP = (CdB_u_LNP*YucudL(1,2)).real();
640 CdB_23i_LNP = (CdB_u_LNP*YucudL(1,2)).imag();
641 CdB_31r_LNP = (CdB_u_LNP*YucudL(2,0)).real();
642 CdB_31i_LNP = (CdB_u_LNP*YucudL(2,0)).imag();
643 CdB_32r_LNP = (CdB_u_LNP*YucudL(2,1)).real();
644 CdB_32i_LNP = (CdB_u_LNP*YucudL(2,1)).imag();
645 CdB_33r_LNP = (CdB_d_LNP*YdddL(2) + CdB_0_LNP*YdL(2) + CdB_u_LNP*YucudL(2,2)).real();
646 CdB_33i_LNP = (CdB_d_LNP*YdddL(2) + CdB_0_LNP*YdL(2) + CdB_u_LNP*YucudL(2,2)).imag();
647
648 CHq1_11r_LNP = (CHq1_0_LNP + CHq1_d_LNP*YddL(0) + CHq1_u_LNP*YucuL(0,0)).real();
649 CHq1_12r_LNP = (CHq1_u_LNP*YucuL(0,1)).real();
650 CHq1_12i_LNP = (CHq1_u_LNP*YucuL(0,1)).imag();
651 CHq1_13r_LNP = (CHq1_u_LNP*YucuL(0,2)).real();
652 CHq1_13i_LNP = (CHq1_u_LNP*YucuL(0,2)).imag();
653 CHq1_22r_LNP = (CHq1_0_LNP + CHq1_d_LNP*YddL(1) + CHq1_u_LNP*YucuL(1,1)).real();
654 CHq1_23r_LNP = (CHq1_u_LNP*YucuL(1,2)).real();
655 CHq1_23i_LNP = (CHq1_u_LNP*YucuL(1,2)).imag();
656 CHq1_33r_LNP = (CHq1_0_LNP + CHq1_d_LNP*YddL(2) + CHq1_u_LNP*YucuL(2,2)).real();
657
658 CHq3_11r_LNP = (CHq3_0_LNP + CHq3_d_LNP*YddL(0) + CHq3_u_LNP*YucuL(0,0)).real();
659 CHq3_12r_LNP = (CHq3_u_LNP*YucuL(0,1)).real();
660 CHq3_12i_LNP = (CHq3_u_LNP*YucuL(0,1)).imag();
661 CHq3_13r_LNP = (CHq3_u_LNP*YucuL(0,2)).real();
662 CHq3_13i_LNP = (CHq3_u_LNP*YucuL(0,2)).imag();
663 CHq3_22r_LNP = (CHq3_0_LNP + CHq3_d_LNP*YddL(1) + CHq3_u_LNP*YucuL(1,1)).real();
664 CHq3_23r_LNP = (CHq3_u_LNP*YucuL(1,2)).real();
665 CHq3_23i_LNP = (CHq3_u_LNP*YucuL(1,2)).imag();
666 CHq3_33r_LNP = (CHq3_0_LNP + CHq3_d_LNP*YddL(2) + CHq3_u_LNP*YucuL(2,2)).real();
667
668 CHu_11r_LNP = (CHu_0_LNP + CHu_u_LNP*YuucL(0,0)).real();
669 CHu_12r_LNP = (CHu_u_LNP*YuucL(0,1)).real();
670 CHu_12i_LNP = (CHu_u_LNP*YuucL(0,1)).imag();
671 CHu_13r_LNP = (CHu_u_LNP*YuucL(0,2)).real();
672 CHu_13i_LNP = (CHu_u_LNP*YuucL(0,2)).imag();
673 CHu_22r_LNP = (CHu_0_LNP + CHu_u_LNP*YuucL(1,1)).real();
674 CHu_23r_LNP = (CHu_u_LNP*YuucL(1,2)).real();
675 CHu_23i_LNP = (CHu_u_LNP*YuucL(1,2)).imag();
676 CHu_33r_LNP = (CHu_0_LNP + CHu_u_LNP*YuucL(2,2)).real();
677
678 CHd_11r_LNP = (CHd_0_LNP + CHd_d_LNP*YddL(0)).real();
679 CHd_22r_LNP = (CHd_0_LNP + CHd_d_LNP*YddL(1)).real();
680 CHd_33r_LNP = (CHd_0_LNP + CHd_d_LNP*YddL(2)).real();
681
682 CHud_11r_LNP = (CHud_ud_LNP*YudL(0,0)).real();
683 CHud_11i_LNP = (CHud_ud_LNP*YudL(0,0)).imag();
684 CHud_12r_LNP = (CHud_ud_LNP*YudL(0,1)).real();
685 CHud_12i_LNP = (CHud_ud_LNP*YudL(0,1)).imag();
686 CHud_13r_LNP = (CHud_ud_LNP*YudL(0,2)).real();
687 CHud_13i_LNP = (CHud_ud_LNP*YudL(0,2)).imag();
688 CHud_21r_LNP = (CHud_ud_LNP*YudL(1,0)).real();
689 CHud_21i_LNP = (CHud_ud_LNP*YudL(1,0)).imag();
690 CHud_22r_LNP = (CHud_ud_LNP*YudL(1,1)).real();
691 CHud_22i_LNP = (CHud_ud_LNP*YudL(1,1)).imag();
692 CHud_23r_LNP = (CHud_ud_LNP*YudL(1,2)).real();
693 CHud_23i_LNP = (CHud_ud_LNP*YudL(1,2)).imag();
694 CHud_31r_LNP = (CHud_ud_LNP*YudL(2,0)).real();
695 CHud_31i_LNP = (CHud_ud_LNP*YudL(2,0)).imag();
696 CHud_32r_LNP = (CHud_ud_LNP*YudL(2,1)).real();
697 CHud_32i_LNP = (CHud_ud_LNP*YudL(2,1)).imag();
698 CHud_33r_LNP = (CHud_ud_LNP*YudL(2,2)).real();
699 CHud_33i_LNP = (CHud_ud_LNP*YudL(2,2)).imag();
700
701 Clq1_1111r_LNP = (Clq1_0_LNP + Clq1_d_LNP*YddL(0) + Clq1_u_LNP*YucuL(0,0)).real();
702 Clq1_1112r_LNP = (Clq1_u_LNP*YucuL(0,1)).real();
703 Clq1_1112i_LNP = (Clq1_u_LNP*YucuL(0,1)).imag();
704 Clq1_1113r_LNP = (Clq1_u_LNP*YucuL(0,2)).real();
705 Clq1_1113i_LNP = (Clq1_u_LNP*YucuL(0,2)).imag();
706 Clq1_1122r_LNP = (Clq1_0_LNP + Clq1_d_LNP*YddL(1) + Clq1_u_LNP*YucuL(1,1)).real();
707 Clq1_1123r_LNP = (Clq1_u_LNP*YucuL(1,2)).real();
708 Clq1_1123i_LNP = (Clq1_u_LNP*YucuL(1,2)).imag();
709 Clq1_1133r_LNP = (Clq1_0_LNP + Clq1_d_LNP*YddL(2) + Clq1_u_LNP*YucuL(2,2)).real();
710 Clq1_2211r_LNP = (Clq1_0_LNP + Clq1_d_LNP*YddL(0) + Clq1_u_LNP*YucuL(0,0)).real();
711 Clq1_2212r_LNP = (Clq1_u_LNP*YucuL(0,1)).real();
712 Clq1_2212i_LNP = (Clq1_u_LNP*YucuL(0,1)).imag();
713 Clq1_2213r_LNP = (Clq1_u_LNP*YucuL(0,2)).real();
714 Clq1_2213i_LNP = (Clq1_u_LNP*YucuL(0,2)).imag();
715 Clq1_2222r_LNP = (Clq1_0_LNP + Clq1_d_LNP*YddL(1) + Clq1_u_LNP*YucuL(1,1)).real();
716 Clq1_2223r_LNP = (Clq1_u_LNP*YucuL(1,2)).real();
717 Clq1_2223i_LNP = (Clq1_u_LNP*YucuL(1,2)).imag();
718 Clq1_2233r_LNP = (Clq1_0_LNP + Clq1_d_LNP*YddL(2) + Clq1_u_LNP*YucuL(2,2)).real();
719 Clq1_3311r_LNP = (Clq1_0_LNP + Clq1_d_LNP*YddL(0) + Clq1_u_LNP*YucuL(0,0)).real();
720 Clq1_3312r_LNP = (Clq1_u_LNP*YucuL(0,1)).real();
721 Clq1_3312i_LNP = (Clq1_u_LNP*YucuL(0,1)).imag();
722 Clq1_3313r_LNP = (Clq1_u_LNP*YucuL(0,2)).real();
723 Clq1_3313i_LNP = (Clq1_u_LNP*YucuL(0,2)).imag();
724 Clq1_3322r_LNP = (Clq1_0_LNP + Clq1_d_LNP*YddL(1) + Clq1_u_LNP*YucuL(1,1)).real();
725 Clq1_3323r_LNP = (Clq1_u_LNP*YucuL(1,2)).real();
726 Clq1_3323i_LNP = (Clq1_u_LNP*YucuL(1,2)).imag();
727 Clq1_3333r_LNP = (Clq1_0_LNP + Clq1_d_LNP*YddL(2) + Clq1_u_LNP*YucuL(2,2)).real();
728
729 Clq3_1111r_LNP = (Clq3_0_LNP + Clq3_d_LNP*YddL(0) + Clq3_u_LNP*YucuL(0,0)).real();
730 Clq3_1112r_LNP = (Clq3_u_LNP*YucuL(0,1)).real();
731 Clq3_1112i_LNP = (Clq3_u_LNP*YucuL(0,1)).imag();
732 Clq3_1113r_LNP = (Clq3_u_LNP*YucuL(0,2)).real();
733 Clq3_1113i_LNP = (Clq3_u_LNP*YucuL(0,2)).imag();
734 Clq3_1122r_LNP = (Clq3_0_LNP + Clq3_d_LNP*YddL(1) + Clq3_u_LNP*YucuL(1,1)).real();
735 Clq3_1123r_LNP = (Clq3_u_LNP*YucuL(1,2)).real();
736 Clq3_1123i_LNP = (Clq3_u_LNP*YucuL(1,2)).imag();
737 Clq3_1133r_LNP = (Clq3_0_LNP + Clq3_d_LNP*YddL(2) + Clq3_u_LNP*YucuL(2,2)).real();
738 Clq3_2211r_LNP = (Clq3_0_LNP + Clq3_d_LNP*YddL(0) + Clq3_u_LNP*YucuL(0,0)).real();
739 Clq3_2212r_LNP = (Clq3_u_LNP*YucuL(0,1)).real();
740 Clq3_2212i_LNP = (Clq3_u_LNP*YucuL(0,1)).imag();
741 Clq3_2213r_LNP = (Clq3_u_LNP*YucuL(0,2)).real();
742 Clq3_2213i_LNP = (Clq3_u_LNP*YucuL(0,2)).imag();
743 Clq3_2222r_LNP = (Clq3_0_LNP + Clq3_d_LNP*YddL(1) + Clq3_u_LNP*YucuL(1,1)).real();
744 Clq3_2223r_LNP = (Clq3_u_LNP*YucuL(1,2)).real();
745 Clq3_2223i_LNP = (Clq3_u_LNP*YucuL(1,2)).imag();
746 Clq3_2233r_LNP = (Clq3_0_LNP + Clq3_d_LNP*YddL(2) + Clq3_u_LNP*YucuL(2,2)).real();
747 Clq3_3311r_LNP = (Clq3_0_LNP + Clq3_d_LNP*YddL(0) + Clq3_u_LNP*YucuL(0,0)).real();
748 Clq3_3312r_LNP = (Clq3_u_LNP*YucuL(0,1)).real();
749 Clq3_3312i_LNP = (Clq3_u_LNP*YucuL(0,1)).imag();
750 Clq3_3313r_LNP = (Clq3_u_LNP*YucuL(0,2)).real();
751 Clq3_3313i_LNP = (Clq3_u_LNP*YucuL(0,2)).imag();
752 Clq3_3322r_LNP = (Clq3_0_LNP + Clq3_d_LNP*YddL(1) + Clq3_u_LNP*YucuL(1,1)).real();
753 Clq3_3323r_LNP = (Clq3_u_LNP*YucuL(1,2)).real();
754 Clq3_3323i_LNP = (Clq3_u_LNP*YucuL(1,2)).imag();
755 Clq3_3333r_LNP = (Clq3_0_LNP + Clq3_d_LNP*YddL(2) + Clq3_u_LNP*YucuL(2,2)).real();
756
757 Cqe_1111r_LNP = (Cqe_0_LNP + Cqe_d_LNP*YddL(0) + Cqe_u_LNP*YucuL(0,0)).real();
758 Cqe_1122r_LNP = (Cqe_0_LNP + Cqe_d_LNP*YddL(0) + Cqe_u_LNP*YucuL(0,0)).real();
759 Cqe_1133r_LNP = (Cqe_0_LNP + Cqe_d_LNP*YddL(0) + Cqe_u_LNP*YucuL(0,0)).real();
760 Cqe_1211r_LNP = (Cqe_u_LNP*YucuL(0,1)).real();
761 Cqe_1211i_LNP = (Cqe_u_LNP*YucuL(0,1)).imag();
762 Cqe_1222r_LNP = (Cqe_u_LNP*YucuL(0,1)).real();
763 Cqe_1222i_LNP = (Cqe_u_LNP*YucuL(0,1)).imag();
764 Cqe_1233r_LNP = (Cqe_u_LNP*YucuL(0,1)).real();
765 Cqe_1233i_LNP = (Cqe_u_LNP*YucuL(0,1)).imag();
766 Cqe_1311r_LNP = (Cqe_u_LNP*YucuL(0,2)).real();
767 Cqe_1311i_LNP = (Cqe_u_LNP*YucuL(0,2)).imag();
768 Cqe_1322r_LNP = (Cqe_u_LNP*YucuL(0,2)).real();
769 Cqe_1322i_LNP = (Cqe_u_LNP*YucuL(0,2)).imag();
770 Cqe_1333r_LNP = (Cqe_u_LNP*YucuL(0,2)).real();
771 Cqe_1333i_LNP = (Cqe_u_LNP*YucuL(0,2)).imag();
772 Cqe_2211r_LNP = (Cqe_0_LNP + Cqe_d_LNP*YddL(1) + Cqe_u_LNP*YucuL(1,1)).real();
773 Cqe_2222r_LNP = (Cqe_0_LNP + Cqe_d_LNP*YddL(1) + Cqe_u_LNP*YucuL(1,1)).real();
774 Cqe_2233r_LNP = (Cqe_0_LNP + Cqe_d_LNP*YddL(1) + Cqe_u_LNP*YucuL(1,1)).real();
775 Cqe_2311r_LNP = (Cqe_u_LNP*YucuL(1,2)).real();
776 Cqe_2311i_LNP = (Cqe_u_LNP*YucuL(1,2)).imag();
777 Cqe_2322r_LNP = (Cqe_u_LNP*YucuL(1,2)).real();
778 Cqe_2322i_LNP = (Cqe_u_LNP*YucuL(1,2)).imag();
779 Cqe_2333r_LNP = (Cqe_u_LNP*YucuL(1,2)).real();
780 Cqe_2333i_LNP = (Cqe_u_LNP*YucuL(1,2)).imag();
781 Cqe_3311r_LNP = (Cqe_0_LNP + Cqe_d_LNP*YddL(2) + Cqe_u_LNP*YucuL(2,2)).real();
782 Cqe_3322r_LNP = (Cqe_0_LNP + Cqe_d_LNP*YddL(2) + Cqe_u_LNP*YucuL(2,2)).real();
783 Cqe_3333r_LNP = (Cqe_0_LNP + Cqe_d_LNP*YddL(2) + Cqe_u_LNP*YucuL(2,2)).real();
784
785 Clu_1111r_LNP = (Clu_0_LNP + Clu_u_LNP*YuucL(0,0)).real();
786 Clu_1112r_LNP = (Clu_u_LNP*YuucL(0,1)).real();
787 Clu_1112i_LNP = (Clu_u_LNP*YuucL(0,1)).imag();
788 Clu_1113r_LNP = (Clu_u_LNP*YuucL(0,2)).real();
789 Clu_1113i_LNP = (Clu_u_LNP*YuucL(0,2)).imag();
790 Clu_1122r_LNP = (Clu_0_LNP + Clu_u_LNP*YuucL(1,1)).real();
791 Clu_1123r_LNP = (Clu_u_LNP*YuucL(1,2)).real();
792 Clu_1123i_LNP = (Clu_u_LNP*YuucL(1,2)).imag();
793 Clu_1133r_LNP = (Clu_0_LNP + Clu_u_LNP*YuucL(2,2)).real();
794 Clu_2211r_LNP = (Clu_0_LNP + Clu_u_LNP*YuucL(0,0)).real();
795 Clu_2212r_LNP = (Clu_u_LNP*YuucL(0,1)).real();
796 Clu_2212i_LNP = (Clu_u_LNP*YuucL(0,1)).imag();
797 Clu_2213r_LNP = (Clu_u_LNP*YuucL(0,2)).real();
798 Clu_2213i_LNP = (Clu_u_LNP*YuucL(0,2)).imag();
799 Clu_2222r_LNP = (Clu_0_LNP + Clu_u_LNP*YuucL(1,1)).real();
800 Clu_2223r_LNP = (Clu_u_LNP*YuucL(1,2)).real();
801 Clu_2223i_LNP = (Clu_u_LNP*YuucL(1,2)).imag();
802 Clu_2233r_LNP = (Clu_0_LNP + Clu_u_LNP*YuucL(2,2)).real();
803 Clu_3311r_LNP = (Clu_0_LNP + Clu_u_LNP*YuucL(0,0)).real();
804 Clu_3312r_LNP = (Clu_u_LNP*YuucL(0,1)).real();
805 Clu_3312i_LNP = (Clu_u_LNP*YuucL(0,1)).imag();
806 Clu_3313r_LNP = (Clu_u_LNP*YuucL(0,2)).real();
807 Clu_3313i_LNP = (Clu_u_LNP*YuucL(0,2)).imag();
808 Clu_3322r_LNP = (Clu_0_LNP + Clu_u_LNP*YuucL(1,1)).real();
809 Clu_3323r_LNP = (Clu_u_LNP*YuucL(1,2)).real();
810 Clu_3323i_LNP = (Clu_u_LNP*YuucL(1,2)).imag();
811 Clu_3333r_LNP = (Clu_0_LNP + Clu_u_LNP*YuucL(2,2)).real();
812
813 Ceu_1111r_LNP = (Ceu_0_LNP + Ceu_u_LNP*YuucL(0,0)).real();
814 Ceu_1112r_LNP = (Ceu_u_LNP*YuucL(0,1)).real();
815 Ceu_1112i_LNP = (Ceu_u_LNP*YuucL(0,1)).imag();
816 Ceu_1113r_LNP = (Ceu_u_LNP*YuucL(0,2)).real();
817 Ceu_1113i_LNP = (Ceu_u_LNP*YuucL(0,2)).imag();
818 Ceu_1122r_LNP = (Ceu_0_LNP + Ceu_u_LNP*YuucL(1,1)).real();
819 Ceu_1123r_LNP = (Ceu_u_LNP*YuucL(1,2)).real();
820 Ceu_1123i_LNP = (Ceu_u_LNP*YuucL(1,2)).imag();
821 Ceu_1133r_LNP = (Ceu_0_LNP + Ceu_u_LNP*YuucL(2,2)).real();
822 Ceu_2211r_LNP = (Ceu_0_LNP + Ceu_u_LNP*YuucL(0,0)).real();
823 Ceu_2212r_LNP = (Ceu_u_LNP*YuucL(0,1)).real();
824 Ceu_2212i_LNP = (Ceu_u_LNP*YuucL(0,1)).imag();
825 Ceu_2213r_LNP = (Ceu_u_LNP*YuucL(0,2)).real();
826 Ceu_2213i_LNP = (Ceu_u_LNP*YuucL(0,2)).imag();
827 Ceu_2222r_LNP = (Ceu_0_LNP + Ceu_u_LNP*YuucL(1,1)).real();
828 Ceu_2223r_LNP = (Ceu_u_LNP*YuucL(1,2)).real();
829 Ceu_2223i_LNP = (Ceu_u_LNP*YuucL(1,2)).imag();
830 Ceu_2233r_LNP = (Ceu_0_LNP + Ceu_u_LNP*YuucL(2,2)).real();
831 Ceu_3311r_LNP = (Ceu_0_LNP + Ceu_u_LNP*YuucL(0,0)).real();
832 Ceu_3312r_LNP = (Ceu_u_LNP*YuucL(0,1)).real();
833 Ceu_3312i_LNP = (Ceu_u_LNP*YuucL(0,1)).imag();
834 Ceu_3313r_LNP = (Ceu_u_LNP*YuucL(0,2)).real();
835 Ceu_3313i_LNP = (Ceu_u_LNP*YuucL(0,2)).imag();
836 Ceu_3322r_LNP = (Ceu_0_LNP + Ceu_u_LNP*YuucL(1,1)).real();
837 Ceu_3323r_LNP = (Ceu_u_LNP*YuucL(1,2)).real();
838 Ceu_3323i_LNP = (Ceu_u_LNP*YuucL(1,2)).imag();
839 Ceu_3333r_LNP = (Ceu_0_LNP + Ceu_u_LNP*YuucL(2,2)).real();
840
841 Cld_1111r_LNP = (Cld_0_LNP + Cld_d_LNP*YddL(0)).real();
842 Cld_1122r_LNP = (Cld_0_LNP + Cld_d_LNP*YddL(1)).real();
843 Cld_1133r_LNP = (Cld_0_LNP + Cld_d_LNP*YddL(2)).real();
844 Cld_2211r_LNP = (Cld_0_LNP + Cld_d_LNP*YddL(0)).real();
845 Cld_2222r_LNP = (Cld_0_LNP + Cld_d_LNP*YddL(1)).real();
846 Cld_2233r_LNP = (Cld_0_LNP + Cld_d_LNP*YddL(2)).real();
847 Cld_3311r_LNP = (Cld_0_LNP + Cld_d_LNP*YddL(0)).real();
848 Cld_3322r_LNP = (Cld_0_LNP + Cld_d_LNP*YddL(1)).real();
849 Cld_3333r_LNP = (Cld_0_LNP + Cld_d_LNP*YddL(2)).real();
850
851 Ced_1111r_LNP = (Ced_0_LNP + Ced_d_LNP*YddL(0)).real();
852 Ced_1122r_LNP = (Ced_0_LNP + Ced_d_LNP*YddL(1)).real();
853 Ced_1133r_LNP = (Ced_0_LNP + Ced_d_LNP*YddL(2)).real();
854 Ced_2211r_LNP = (Ced_0_LNP + Ced_d_LNP*YddL(0)).real();
855 Ced_2222r_LNP = (Ced_0_LNP + Ced_d_LNP*YddL(1)).real();
856 Ced_2233r_LNP = (Ced_0_LNP + Ced_d_LNP*YddL(2)).real();
857 Ced_3311r_LNP = (Ced_0_LNP + Ced_d_LNP*YddL(0)).real();
858 Ced_3322r_LNP = (Ced_0_LNP + Ced_d_LNP*YddL(1)).real();
859 Ced_3333r_LNP = (Ced_0_LNP + Ced_d_LNP*YddL(2)).real();
860
861 Cqq1_1111r_LNP = (2*Cqq1_00_LNP + 2*Cqq1_0d_LNP*YddL(0) + 2*Cqq1_d0_LNP*YddL(0) + 2*Cqq1_dd_LNP*YddL(0)*YddL(0) + 2*Cqq1_0u_LNP*YucuL(0,0) + 2*Cqq1_u0_LNP*YucuL(0,0) + 2*Cqq1_du_LNP*YddL(0)*YucuL(0,0) + 2*Cqq1_ud_LNP*YddL(0)*YucuL(0,0) + 2*Cqq1_uu_LNP*YucuL(0,0)*YucuL(0,0)).real();
862 Cqq1_1112r_LNP = (Cqq1_0u_LNP*YucuL(0,1) + Cqq1_u0_LNP*YucuL(0,1) + Cqq1_du_LNP*YddL(0)*YucuL(0,1) + Cqq1_ud_LNP*YddL(0)*YucuL(0,1) + 2*Cqq1_uu_LNP*YucuL(0,0)*YucuL(0,1)).real();
863 Cqq1_1112i_LNP = (Cqq1_0u_LNP*YucuL(0,1) + Cqq1_u0_LNP*YucuL(0,1) + Cqq1_du_LNP*YddL(0)*YucuL(0,1) + Cqq1_ud_LNP*YddL(0)*YucuL(0,1) + 2*Cqq1_uu_LNP*YucuL(0,0)*YucuL(0,1)).imag();
864 Cqq1_1113r_LNP = (Cqq1_0u_LNP*YucuL(0,2) + Cqq1_u0_LNP*YucuL(0,2) + Cqq1_du_LNP*YddL(0)*YucuL(0,2) + Cqq1_ud_LNP*YddL(0)*YucuL(0,2) + 2*Cqq1_uu_LNP*YucuL(0,0)*YucuL(0,2)).real();
865 Cqq1_1113i_LNP = (Cqq1_0u_LNP*YucuL(0,2) + Cqq1_u0_LNP*YucuL(0,2) + Cqq1_du_LNP*YddL(0)*YucuL(0,2) + Cqq1_ud_LNP*YddL(0)*YucuL(0,2) + 2*Cqq1_uu_LNP*YucuL(0,0)*YucuL(0,2)).imag();
866 Cqq1_1122r_LNP = (Cqq1_00_LNP + Cqq1_d0_LNP*YddL(0) + Cqq1_0d_LNP*YddL(1) + Cqq1_dd_LNP*YddL(0)*YddL(1) + Cqq1_u0_LNP*YucuL(0,0) + Cqq1_ud_LNP*YddL(1)*YucuL(0,0) + Cqq1_uu_LNP*YucuL(0,1)*YucuL(1,0) + Cqq1_0u_LNP*YucuL(1,1) + Cqq1_du_LNP*YddL(0)*YucuL(1,1) + Cqq1_uu_LNP*YucuL(0,0)*YucuL(1,1)).real();
867 Cqq1_1123r_LNP = (Cqq1_uu_LNP*YucuL(0,2)*YucuL(1,0) + Cqq1_0u_LNP*YucuL(1,2) + Cqq1_du_LNP*YddL(0)*YucuL(1,2) + Cqq1_uu_LNP*YucuL(0,0)*YucuL(1,2)).real();
868 Cqq1_1123i_LNP = (Cqq1_uu_LNP*YucuL(0,2)*YucuL(1,0) + Cqq1_0u_LNP*YucuL(1,2) + Cqq1_du_LNP*YddL(0)*YucuL(1,2) + Cqq1_uu_LNP*YucuL(0,0)*YucuL(1,2)).imag();
869 Cqq1_1133r_LNP = (Cqq1_00_LNP + Cqq1_d0_LNP*YddL(0) + Cqq1_0d_LNP*YddL(2) + Cqq1_dd_LNP*YddL(0)*YddL(2) + Cqq1_u0_LNP*YucuL(0,0) + Cqq1_ud_LNP*YddL(2)*YucuL(0,0) + Cqq1_uu_LNP*YucuL(0,2)*YucuL(2,0) + Cqq1_0u_LNP*YucuL(2,2) + Cqq1_du_LNP*YddL(0)*YucuL(2,2) + Cqq1_uu_LNP*YucuL(0,0)*YucuL(2,2)).real();
870 Cqq1_1212r_LNP = (2*Cqq1_uu_LNP*YucuL(0,1)*YucuL(0,1)).real();
871 Cqq1_1212i_LNP = (2*Cqq1_uu_LNP*YucuL(0,1)*YucuL(0,1)).imag();
872 Cqq1_1213r_LNP = (2*Cqq1_uu_LNP*YucuL(0,1)*YucuL(0,2)).real();
873 Cqq1_1213i_LNP = (2*Cqq1_uu_LNP*YucuL(0,1)*YucuL(0,2)).imag();
874 Cqq1_1221r_LNP = (Cqq1_00_LNP + Cqq1_d0_LNP*YddL(0) + Cqq1_0d_LNP*YddL(1) + Cqq1_dd_LNP*YddL(0)*YddL(1) + Cqq1_u0_LNP*YucuL(0,0) + Cqq1_ud_LNP*YddL(1)*YucuL(0,0) + Cqq1_uu_LNP*YucuL(0,1)*YucuL(1,0) + Cqq1_0u_LNP*YucuL(1,1) + Cqq1_du_LNP*YddL(0)*YucuL(1,1) + Cqq1_uu_LNP*YucuL(0,0)*YucuL(1,1)).real();
875 Cqq1_1222r_LNP = (2*Cqq1_u0_LNP*YucuL(0,1) + 2*Cqq1_ud_LNP*YddL(1)*YucuL(0,1) + 2*Cqq1_uu_LNP*YucuL(0,1)*YucuL(1,1)).real();
876 Cqq1_1222i_LNP = (2*Cqq1_u0_LNP*YucuL(0,1) + 2*Cqq1_ud_LNP*YddL(1)*YucuL(0,1) + 2*Cqq1_uu_LNP*YucuL(0,1)*YucuL(1,1)).imag();
877 Cqq1_1223r_LNP = (Cqq1_u0_LNP*YucuL(0,2) + Cqq1_ud_LNP*YddL(1)*YucuL(0,2) + Cqq1_uu_LNP*YucuL(0,2)*YucuL(1,1) + Cqq1_uu_LNP*YucuL(0,1)*YucuL(1,2)).real();
878 Cqq1_1223i_LNP = (Cqq1_u0_LNP*YucuL(0,2) + Cqq1_ud_LNP*YddL(1)*YucuL(0,2) + Cqq1_uu_LNP*YucuL(0,2)*YucuL(1,1) + Cqq1_uu_LNP*YucuL(0,1)*YucuL(1,2)).imag();
879 Cqq1_1231r_LNP = (Cqq1_uu_LNP*YucuL(0,1)*YucuL(2,0) + Cqq1_0u_LNP*YucuL(2,1) + Cqq1_du_LNP*YddL(0)*YucuL(2,1) + Cqq1_uu_LNP*YucuL(0,0)*YucuL(2,1)).real();
880 Cqq1_1231i_LNP = (Cqq1_uu_LNP*YucuL(0,1)*YucuL(2,0) + Cqq1_0u_LNP*YucuL(2,1) + Cqq1_du_LNP*YddL(0)*YucuL(2,1) + Cqq1_uu_LNP*YucuL(0,0)*YucuL(2,1)).imag();
881 Cqq1_1232r_LNP = (2*Cqq1_uu_LNP*YucuL(0,1)*YucuL(2,1)).real();
882 Cqq1_1232i_LNP = (2*Cqq1_uu_LNP*YucuL(0,1)*YucuL(2,1)).imag();
883 Cqq1_1233r_LNP = (Cqq1_u0_LNP*YucuL(0,1) + Cqq1_ud_LNP*YddL(2)*YucuL(0,1) + Cqq1_uu_LNP*YucuL(0,2)*YucuL(2,1) + Cqq1_uu_LNP*YucuL(0,1)*YucuL(2,2)).real();
884 Cqq1_1233i_LNP = (Cqq1_u0_LNP*YucuL(0,1) + Cqq1_ud_LNP*YddL(2)*YucuL(0,1) + Cqq1_uu_LNP*YucuL(0,2)*YucuL(2,1) + Cqq1_uu_LNP*YucuL(0,1)*YucuL(2,2)).imag();
885 Cqq1_1313r_LNP = (2*Cqq1_uu_LNP*YucuL(0,2)*YucuL(0,2)).real();
886 Cqq1_1313i_LNP = (2*Cqq1_uu_LNP*YucuL(0,2)*YucuL(0,2)).imag();
887 Cqq1_1322r_LNP = (Cqq1_u0_LNP*YucuL(0,2) + Cqq1_ud_LNP*YddL(1)*YucuL(0,2) + Cqq1_uu_LNP*YucuL(0,2)*YucuL(1,1) + Cqq1_uu_LNP*YucuL(0,1)*YucuL(1,2)).real();
888 Cqq1_1322i_LNP = (Cqq1_u0_LNP*YucuL(0,2) + Cqq1_ud_LNP*YddL(1)*YucuL(0,2) + Cqq1_uu_LNP*YucuL(0,2)*YucuL(1,1) + Cqq1_uu_LNP*YucuL(0,1)*YucuL(1,2)).imag();
889 Cqq1_1323r_LNP = (2*Cqq1_uu_LNP*YucuL(0,2)*YucuL(1,2)).real();
890 Cqq1_1323i_LNP = (2*Cqq1_uu_LNP*YucuL(0,2)*YucuL(1,2)).imag();
891 Cqq1_1331r_LNP = (Cqq1_00_LNP + Cqq1_d0_LNP*YddL(0) + Cqq1_0d_LNP*YddL(2) + Cqq1_dd_LNP*YddL(0)*YddL(2) + Cqq1_u0_LNP*YucuL(0,0) + Cqq1_ud_LNP*YddL(2)*YucuL(0,0) + Cqq1_uu_LNP*YucuL(0,2)*YucuL(2,0) + Cqq1_0u_LNP*YucuL(2,2) + Cqq1_du_LNP*YddL(0)*YucuL(2,2) + Cqq1_uu_LNP*YucuL(0,0)*YucuL(2,2)).real();
892 Cqq1_1332r_LNP = (Cqq1_u0_LNP*YucuL(0,1) + Cqq1_ud_LNP*YddL(2)*YucuL(0,1) + Cqq1_uu_LNP*YucuL(0,2)*YucuL(2,1) + Cqq1_uu_LNP*YucuL(0,1)*YucuL(2,2)).real();
893 Cqq1_1332i_LNP = (Cqq1_u0_LNP*YucuL(0,1) + Cqq1_ud_LNP*YddL(2)*YucuL(0,1) + Cqq1_uu_LNP*YucuL(0,2)*YucuL(2,1) + Cqq1_uu_LNP*YucuL(0,1)*YucuL(2,2)).imag();
894 Cqq1_1333r_LNP = (2*Cqq1_u0_LNP*YucuL(0,2) + 2*Cqq1_ud_LNP*YddL(2)*YucuL(0,2) + 2*Cqq1_uu_LNP*YucuL(0,2)*YucuL(2,2)).real();
895 Cqq1_1333i_LNP = (2*Cqq1_u0_LNP*YucuL(0,2) + 2*Cqq1_ud_LNP*YddL(2)*YucuL(0,2) + 2*Cqq1_uu_LNP*YucuL(0,2)*YucuL(2,2)).imag();
896 Cqq1_2222r_LNP = (2*Cqq1_00_LNP + 2*Cqq1_0d_LNP*YddL(1) + 2*Cqq1_d0_LNP*YddL(1) + 2*Cqq1_dd_LNP*YddL(1)*YddL(1) + 2*Cqq1_0u_LNP*YucuL(1,1) + 2*Cqq1_u0_LNP*YucuL(1,1) + 2*Cqq1_du_LNP*YddL(1)*YucuL(1,1) + 2*Cqq1_ud_LNP*YddL(1)*YucuL(1,1) + 2*Cqq1_uu_LNP*YucuL(1,1)*YucuL(1,1)).real();
897 Cqq1_2223r_LNP = (Cqq1_0u_LNP*YucuL(1,2) + Cqq1_u0_LNP*YucuL(1,2) + Cqq1_du_LNP*YddL(1)*YucuL(1,2) + Cqq1_ud_LNP*YddL(1)*YucuL(1,2) + 2*Cqq1_uu_LNP*YucuL(1,1)*YucuL(1,2)).real();
898 Cqq1_2223i_LNP = (Cqq1_0u_LNP*YucuL(1,2) + Cqq1_u0_LNP*YucuL(1,2) + Cqq1_du_LNP*YddL(1)*YucuL(1,2) + Cqq1_ud_LNP*YddL(1)*YucuL(1,2) + 2*Cqq1_uu_LNP*YucuL(1,1)*YucuL(1,2)).imag();
899 Cqq1_2233r_LNP = (Cqq1_00_LNP + Cqq1_d0_LNP*YddL(1) + Cqq1_0d_LNP*YddL(2) + Cqq1_dd_LNP*YddL(1)*YddL(2) + Cqq1_u0_LNP*YucuL(1,1) + Cqq1_ud_LNP*YddL(2)*YucuL(1,1) + Cqq1_uu_LNP*YucuL(1,2)*YucuL(2,1) + Cqq1_0u_LNP*YucuL(2,2) + Cqq1_du_LNP*YddL(1)*YucuL(2,2) + Cqq1_uu_LNP*YucuL(1,1)*YucuL(2,2)).real();
900 Cqq1_2323r_LNP = (2*Cqq1_uu_LNP*YucuL(1,2)*YucuL(1,2)).real();
901 Cqq1_2323i_LNP = (2*Cqq1_uu_LNP*YucuL(1,2)*YucuL(1,2)).imag();
902 Cqq1_2332r_LNP = (Cqq1_00_LNP + Cqq1_d0_LNP*YddL(1) + Cqq1_0d_LNP*YddL(2) + Cqq1_dd_LNP*YddL(1)*YddL(2) + Cqq1_u0_LNP*YucuL(1,1) + Cqq1_ud_LNP*YddL(2)*YucuL(1,1) + Cqq1_uu_LNP*YucuL(1,2)*YucuL(2,1) + Cqq1_0u_LNP*YucuL(2,2) + Cqq1_du_LNP*YddL(1)*YucuL(2,2) + Cqq1_uu_LNP*YucuL(1,1)*YucuL(2,2)).real();
903 Cqq1_2333r_LNP = (2*Cqq1_u0_LNP*YucuL(1,2) + 2*Cqq1_ud_LNP*YddL(2)*YucuL(1,2) + 2*Cqq1_uu_LNP*YucuL(1,2)*YucuL(2,2)).real();
904 Cqq1_2333i_LNP = (2*Cqq1_u0_LNP*YucuL(1,2) + 2*Cqq1_ud_LNP*YddL(2)*YucuL(1,2) + 2*Cqq1_uu_LNP*YucuL(1,2)*YucuL(2,2)).imag();
905 Cqq1_3333r_LNP = (2*Cqq1_00_LNP + 2*Cqq1_0d_LNP*YddL(2) + 2*Cqq1_d0_LNP*YddL(2) + 2*Cqq1_dd_LNP*YddL(2)*YddL(2) + 2*Cqq1_0u_LNP*YucuL(2,2) + 2*Cqq1_u0_LNP*YucuL(2,2) + 2*Cqq1_du_LNP*YddL(2)*YucuL(2,2) + 2*Cqq1_ud_LNP*YddL(2)*YucuL(2,2) + 2*Cqq1_uu_LNP*YucuL(2,2)*YucuL(2,2)).real();
906
907 Cqq3_1111r_LNP = (2*Cqq3_00_LNP + 2*Cqq3_0d_LNP*YddL(0) + 2*Cqq3_d0_LNP*YddL(0) + 2*Cqq3_dd_LNP*YddL(0)*YddL(0) + 2*Cqq3_0u_LNP*YucuL(0,0) + 2*Cqq3_u0_LNP*YucuL(0,0) + 2*Cqq3_du_LNP*YddL(0)*YucuL(0,0) + 2*Cqq3_ud_LNP*YddL(0)*YucuL(0,0) + 2*Cqq3_uu_LNP*YucuL(0,0)*YucuL(0,0)).real();
908 Cqq3_1112r_LNP = (Cqq3_0u_LNP*YucuL(0,1) + Cqq3_u0_LNP*YucuL(0,1) + Cqq3_du_LNP*YddL(0)*YucuL(0,1) + Cqq3_ud_LNP*YddL(0)*YucuL(0,1) + 2*Cqq3_uu_LNP*YucuL(0,0)*YucuL(0,1)).real();
909 Cqq3_1112i_LNP = (Cqq3_0u_LNP*YucuL(0,1) + Cqq3_u0_LNP*YucuL(0,1) + Cqq3_du_LNP*YddL(0)*YucuL(0,1) + Cqq3_ud_LNP*YddL(0)*YucuL(0,1) + 2*Cqq3_uu_LNP*YucuL(0,0)*YucuL(0,1)).imag();
910 Cqq3_1113r_LNP = (Cqq3_0u_LNP*YucuL(0,2) + Cqq3_u0_LNP*YucuL(0,2) + Cqq3_du_LNP*YddL(0)*YucuL(0,2) + Cqq3_ud_LNP*YddL(0)*YucuL(0,2) + 2*Cqq3_uu_LNP*YucuL(0,0)*YucuL(0,2)).real();
911 Cqq3_1113i_LNP = (Cqq3_0u_LNP*YucuL(0,2) + Cqq3_u0_LNP*YucuL(0,2) + Cqq3_du_LNP*YddL(0)*YucuL(0,2) + Cqq3_ud_LNP*YddL(0)*YucuL(0,2) + 2*Cqq3_uu_LNP*YucuL(0,0)*YucuL(0,2)).imag();
912 Cqq3_1122r_LNP = (Cqq3_00_LNP + Cqq3_d0_LNP*YddL(0) + Cqq3_0d_LNP*YddL(1) + Cqq3_dd_LNP*YddL(0)*YddL(1) + Cqq3_u0_LNP*YucuL(0,0) + Cqq3_ud_LNP*YddL(1)*YucuL(0,0) + Cqq3_uu_LNP*YucuL(0,1)*YucuL(1,0) + Cqq3_0u_LNP*YucuL(1,1) + Cqq3_du_LNP*YddL(0)*YucuL(1,1) + Cqq3_uu_LNP*YucuL(0,0)*YucuL(1,1)).real();
913 Cqq3_1123r_LNP = (Cqq3_uu_LNP*YucuL(0,2)*YucuL(1,0) + Cqq3_0u_LNP*YucuL(1,2) + Cqq3_du_LNP*YddL(0)*YucuL(1,2) + Cqq3_uu_LNP*YucuL(0,0)*YucuL(1,2)).real();
914 Cqq3_1123i_LNP = (Cqq3_uu_LNP*YucuL(0,2)*YucuL(1,0) + Cqq3_0u_LNP*YucuL(1,2) + Cqq3_du_LNP*YddL(0)*YucuL(1,2) + Cqq3_uu_LNP*YucuL(0,0)*YucuL(1,2)).imag();
915 Cqq3_1133r_LNP = (Cqq3_00_LNP + Cqq3_d0_LNP*YddL(0) + Cqq3_0d_LNP*YddL(2) + Cqq3_dd_LNP*YddL(0)*YddL(2) + Cqq3_u0_LNP*YucuL(0,0) + Cqq3_ud_LNP*YddL(2)*YucuL(0,0) + Cqq3_uu_LNP*YucuL(0,2)*YucuL(2,0) + Cqq3_0u_LNP*YucuL(2,2) + Cqq3_du_LNP*YddL(0)*YucuL(2,2) + Cqq3_uu_LNP*YucuL(0,0)*YucuL(2,2)).real();
916 Cqq3_1212r_LNP = (2*Cqq3_uu_LNP*YucuL(0,1)*YucuL(0,1)).real();
917 Cqq3_1212i_LNP = (2*Cqq3_uu_LNP*YucuL(0,1)*YucuL(0,1)).imag();
918 Cqq3_1213r_LNP = (2*Cqq3_uu_LNP*YucuL(0,1)*YucuL(0,2)).real();
919 Cqq3_1213i_LNP = (2*Cqq3_uu_LNP*YucuL(0,1)*YucuL(0,2)).imag();
920 Cqq3_1221r_LNP = (Cqq3_00_LNP + Cqq3_d0_LNP*YddL(0) + Cqq3_0d_LNP*YddL(1) + Cqq3_dd_LNP*YddL(0)*YddL(1) + Cqq3_u0_LNP*YucuL(0,0) + Cqq3_ud_LNP*YddL(1)*YucuL(0,0) + Cqq3_uu_LNP*YucuL(0,1)*YucuL(1,0) + Cqq3_0u_LNP*YucuL(1,1) + Cqq3_du_LNP*YddL(0)*YucuL(1,1) + Cqq3_uu_LNP*YucuL(0,0)*YucuL(1,1)).real();
921 Cqq3_1222r_LNP = (2*Cqq3_u0_LNP*YucuL(0,1) + 2*Cqq3_ud_LNP*YddL(1)*YucuL(0,1) + 2*Cqq3_uu_LNP*YucuL(0,1)*YucuL(1,1)).real();
922 Cqq3_1222i_LNP = (2*Cqq3_u0_LNP*YucuL(0,1) + 2*Cqq3_ud_LNP*YddL(1)*YucuL(0,1) + 2*Cqq3_uu_LNP*YucuL(0,1)*YucuL(1,1)).imag();
923 Cqq3_1223r_LNP = (Cqq3_u0_LNP*YucuL(0,2) + Cqq3_ud_LNP*YddL(1)*YucuL(0,2) + Cqq3_uu_LNP*YucuL(0,2)*YucuL(1,1) + Cqq3_uu_LNP*YucuL(0,1)*YucuL(1,2)).real();
924 Cqq3_1223i_LNP = (Cqq3_u0_LNP*YucuL(0,2) + Cqq3_ud_LNP*YddL(1)*YucuL(0,2) + Cqq3_uu_LNP*YucuL(0,2)*YucuL(1,1) + Cqq3_uu_LNP*YucuL(0,1)*YucuL(1,2)).imag();
925 Cqq3_1231r_LNP = (Cqq3_uu_LNP*YucuL(0,1)*YucuL(2,0) + Cqq3_0u_LNP*YucuL(2,1) + Cqq3_du_LNP*YddL(0)*YucuL(2,1) + Cqq3_uu_LNP*YucuL(0,0)*YucuL(2,1)).real();
926 Cqq3_1231i_LNP = (Cqq3_uu_LNP*YucuL(0,1)*YucuL(2,0) + Cqq3_0u_LNP*YucuL(2,1) + Cqq3_du_LNP*YddL(0)*YucuL(2,1) + Cqq3_uu_LNP*YucuL(0,0)*YucuL(2,1)).imag();
927 Cqq3_1232r_LNP = (2*Cqq3_uu_LNP*YucuL(0,1)*YucuL(2,1)).real();
928 Cqq3_1232i_LNP = (2*Cqq3_uu_LNP*YucuL(0,1)*YucuL(2,1)).imag();
929 Cqq3_1233r_LNP = (Cqq3_u0_LNP*YucuL(0,1) + Cqq3_ud_LNP*YddL(2)*YucuL(0,1) + Cqq3_uu_LNP*YucuL(0,2)*YucuL(2,1) + Cqq3_uu_LNP*YucuL(0,1)*YucuL(2,2)).real();
930 Cqq3_1233i_LNP = (Cqq3_u0_LNP*YucuL(0,1) + Cqq3_ud_LNP*YddL(2)*YucuL(0,1) + Cqq3_uu_LNP*YucuL(0,2)*YucuL(2,1) + Cqq3_uu_LNP*YucuL(0,1)*YucuL(2,2)).imag();
931 Cqq3_1313r_LNP = (2*Cqq3_uu_LNP*YucuL(0,2)*YucuL(0,2)).real();
932 Cqq3_1313i_LNP = (2*Cqq3_uu_LNP*YucuL(0,2)*YucuL(0,2)).imag();
933 Cqq3_1322r_LNP = (Cqq3_u0_LNP*YucuL(0,2) + Cqq3_ud_LNP*YddL(1)*YucuL(0,2) + Cqq3_uu_LNP*YucuL(0,2)*YucuL(1,1) + Cqq3_uu_LNP*YucuL(0,1)*YucuL(1,2)).real();
934 Cqq3_1322i_LNP = (Cqq3_u0_LNP*YucuL(0,2) + Cqq3_ud_LNP*YddL(1)*YucuL(0,2) + Cqq3_uu_LNP*YucuL(0,2)*YucuL(1,1) + Cqq3_uu_LNP*YucuL(0,1)*YucuL(1,2)).imag();
935 Cqq3_1323r_LNP = (2*Cqq3_uu_LNP*YucuL(0,2)*YucuL(1,2)).real();
936 Cqq3_1323i_LNP = (2*Cqq3_uu_LNP*YucuL(0,2)*YucuL(1,2)).imag();
937 Cqq3_1331r_LNP = (Cqq3_00_LNP + Cqq3_d0_LNP*YddL(0) + Cqq3_0d_LNP*YddL(2) + Cqq3_dd_LNP*YddL(0)*YddL(2) + Cqq3_u0_LNP*YucuL(0,0) + Cqq3_ud_LNP*YddL(2)*YucuL(0,0) + Cqq3_uu_LNP*YucuL(0,2)*YucuL(2,0) + Cqq3_0u_LNP*YucuL(2,2) + Cqq3_du_LNP*YddL(0)*YucuL(2,2) + Cqq3_uu_LNP*YucuL(0,0)*YucuL(2,2)).real();
938 Cqq3_1332r_LNP = (Cqq3_u0_LNP*YucuL(0,1) + Cqq3_ud_LNP*YddL(2)*YucuL(0,1) + Cqq3_uu_LNP*YucuL(0,2)*YucuL(2,1) + Cqq3_uu_LNP*YucuL(0,1)*YucuL(2,2)).real();
939 Cqq3_1332i_LNP = (Cqq3_u0_LNP*YucuL(0,1) + Cqq3_ud_LNP*YddL(2)*YucuL(0,1) + Cqq3_uu_LNP*YucuL(0,2)*YucuL(2,1) + Cqq3_uu_LNP*YucuL(0,1)*YucuL(2,2)).imag();
940 Cqq3_1333r_LNP = (2*Cqq3_u0_LNP*YucuL(0,2) + 2*Cqq3_ud_LNP*YddL(2)*YucuL(0,2) + 2*Cqq3_uu_LNP*YucuL(0,2)*YucuL(2,2)).real();
941 Cqq3_1333i_LNP = (2*Cqq3_u0_LNP*YucuL(0,2) + 2*Cqq3_ud_LNP*YddL(2)*YucuL(0,2) + 2*Cqq3_uu_LNP*YucuL(0,2)*YucuL(2,2)).imag();
942 Cqq3_2222r_LNP = (2*Cqq3_00_LNP + 2*Cqq3_0d_LNP*YddL(1) + 2*Cqq3_d0_LNP*YddL(1) + 2*Cqq3_dd_LNP*YddL(1)*YddL(1) + 2*Cqq3_0u_LNP*YucuL(1,1) + 2*Cqq3_u0_LNP*YucuL(1,1) + 2*Cqq3_du_LNP*YddL(1)*YucuL(1,1) + 2*Cqq3_ud_LNP*YddL(1)*YucuL(1,1) + 2*Cqq3_uu_LNP*YucuL(1,1)*YucuL(1,1)).real();
943 Cqq3_2223r_LNP = (Cqq3_0u_LNP*YucuL(1,2) + Cqq3_u0_LNP*YucuL(1,2) + Cqq3_du_LNP*YddL(1)*YucuL(1,2) + Cqq3_ud_LNP*YddL(1)*YucuL(1,2) + 2*Cqq3_uu_LNP*YucuL(1,1)*YucuL(1,2)).real();
944 Cqq3_2223i_LNP = (Cqq3_0u_LNP*YucuL(1,2) + Cqq3_u0_LNP*YucuL(1,2) + Cqq3_du_LNP*YddL(1)*YucuL(1,2) + Cqq3_ud_LNP*YddL(1)*YucuL(1,2) + 2*Cqq3_uu_LNP*YucuL(1,1)*YucuL(1,2)).imag();
945 Cqq3_2233r_LNP = (Cqq3_00_LNP + Cqq3_d0_LNP*YddL(1) + Cqq3_0d_LNP*YddL(2) + Cqq3_dd_LNP*YddL(1)*YddL(2) + Cqq3_u0_LNP*YucuL(1,1) + Cqq3_ud_LNP*YddL(2)*YucuL(1,1) + Cqq3_uu_LNP*YucuL(1,2)*YucuL(2,1) + Cqq3_0u_LNP*YucuL(2,2) + Cqq3_du_LNP*YddL(1)*YucuL(2,2) + Cqq3_uu_LNP*YucuL(1,1)*YucuL(2,2)).real();
946 Cqq3_2323r_LNP = (2*Cqq3_uu_LNP*YucuL(1,2)*YucuL(1,2)).real();
947 Cqq3_2323i_LNP = (2*Cqq3_uu_LNP*YucuL(1,2)*YucuL(1,2)).imag();
948 Cqq3_2332r_LNP = (Cqq3_00_LNP + Cqq3_d0_LNP*YddL(1) + Cqq3_0d_LNP*YddL(2) + Cqq3_dd_LNP*YddL(1)*YddL(2) + Cqq3_u0_LNP*YucuL(1,1) + Cqq3_ud_LNP*YddL(2)*YucuL(1,1) + Cqq3_uu_LNP*YucuL(1,2)*YucuL(2,1) + Cqq3_0u_LNP*YucuL(2,2) + Cqq3_du_LNP*YddL(1)*YucuL(2,2) + Cqq3_uu_LNP*YucuL(1,1)*YucuL(2,2)).real();
949 Cqq3_2333r_LNP = (2*Cqq3_u0_LNP*YucuL(1,2) + 2*Cqq3_ud_LNP*YddL(2)*YucuL(1,2) + 2*Cqq3_uu_LNP*YucuL(1,2)*YucuL(2,2)).real();
950 Cqq3_2333i_LNP = (2*Cqq3_u0_LNP*YucuL(1,2) + 2*Cqq3_ud_LNP*YddL(2)*YucuL(1,2) + 2*Cqq3_uu_LNP*YucuL(1,2)*YucuL(2,2)).imag();
951 Cqq3_3333r_LNP = (2*Cqq3_00_LNP + 2*Cqq3_0d_LNP*YddL(2) + 2*Cqq3_d0_LNP*YddL(2) + 2*Cqq3_dd_LNP*YddL(2)*YddL(2) + 2*Cqq3_0u_LNP*YucuL(2,2) + 2*Cqq3_u0_LNP*YucuL(2,2) + 2*Cqq3_du_LNP*YddL(2)*YucuL(2,2) + 2*Cqq3_ud_LNP*YddL(2)*YucuL(2,2) + 2*Cqq3_uu_LNP*YucuL(2,2)*YucuL(2,2)).real();
952
953 Cuu_1111r_LNP = (2*Cuu_00_LNP + 2*Cuu_0u_LNP*YuucL(0,0) + 2*Cuu_u0_LNP*YuucL(0,0) + 2*Cuu_uu_LNP*YuucL(0,0)*YuucL(0,0)).real();
954 Cuu_1112r_LNP = (Cuu_0u_LNP*YuucL(0,1) + Cuu_u0_LNP*YuucL(0,1) + 2*Cuu_uu_LNP*YuucL(0,0)*YuucL(0,1)).real();
955 Cuu_1112i_LNP = (Cuu_0u_LNP*YuucL(0,1) + Cuu_u0_LNP*YuucL(0,1) + 2*Cuu_uu_LNP*YuucL(0,0)*YuucL(0,1)).imag();
956 Cuu_1113r_LNP = (Cuu_0u_LNP*YuucL(0,2) + Cuu_u0_LNP*YuucL(0,2) + 2*Cuu_uu_LNP*YuucL(0,0)*YuucL(0,2)).real();
957 Cuu_1113i_LNP = (Cuu_0u_LNP*YuucL(0,2) + Cuu_u0_LNP*YuucL(0,2) + 2*Cuu_uu_LNP*YuucL(0,0)*YuucL(0,2)).imag();
958 Cuu_1122r_LNP = (Cuu_00_LNP + Cuu_u0_LNP*YuucL(0,0) + Cuu_uu_LNP*YuucL(0,1)*YuucL(1,0) + Cuu_0u_LNP*YuucL(1,1) + Cuu_uu_LNP*YuucL(0,0)*YuucL(1,1)).real();
959 Cuu_1123r_LNP = (Cuu_uu_LNP*YuucL(0,2)*YuucL(1,0) + Cuu_0u_LNP*YuucL(1,2) + Cuu_uu_LNP*YuucL(0,0)*YuucL(1,2)).real();
960 Cuu_1123i_LNP = (Cuu_uu_LNP*YuucL(0,2)*YuucL(1,0) + Cuu_0u_LNP*YuucL(1,2) + Cuu_uu_LNP*YuucL(0,0)*YuucL(1,2)).imag();
961 Cuu_1133r_LNP = (Cuu_00_LNP + Cuu_u0_LNP*YuucL(0,0) + Cuu_uu_LNP*YuucL(0,2)*YuucL(2,0) + Cuu_0u_LNP*YuucL(2,2) + Cuu_uu_LNP*YuucL(0,0)*YuucL(2,2)).real();
962 Cuu_1212r_LNP = (2*Cuu_uu_LNP*YuucL(0,1)*YuucL(0,1)).real();
963 Cuu_1212i_LNP = (2*Cuu_uu_LNP*YuucL(0,1)*YuucL(0,1)).imag();
964 Cuu_1213r_LNP = (2*Cuu_uu_LNP*YuucL(0,1)*YuucL(0,2)).real();
965 Cuu_1213i_LNP = (2*Cuu_uu_LNP*YuucL(0,1)*YuucL(0,2)).imag();
966 Cuu_1221r_LNP = (Cuu_00_LNP + Cuu_u0_LNP*YuucL(0,0) + Cuu_uu_LNP*YuucL(0,1)*YuucL(1,0) + Cuu_0u_LNP*YuucL(1,1) + Cuu_uu_LNP*YuucL(0,0)*YuucL(1,1)).real();
967 Cuu_1222r_LNP = (2*Cuu_u0_LNP*YuucL(0,1) + 2*Cuu_uu_LNP*YuucL(0,1)*YuucL(1,1)).real();
968 Cuu_1222i_LNP = (2*Cuu_u0_LNP*YuucL(0,1) + 2*Cuu_uu_LNP*YuucL(0,1)*YuucL(1,1)).imag();
969 Cuu_1223r_LNP = (Cuu_u0_LNP*YuucL(0,2) + Cuu_uu_LNP*YuucL(0,2)*YuucL(1,1) + Cuu_uu_LNP*YuucL(0,1)*YuucL(1,2)).real();
970 Cuu_1223i_LNP = (Cuu_u0_LNP*YuucL(0,2) + Cuu_uu_LNP*YuucL(0,2)*YuucL(1,1) + Cuu_uu_LNP*YuucL(0,1)*YuucL(1,2)).imag();
971 Cuu_1231r_LNP = (Cuu_uu_LNP*YuucL(0,1)*YuucL(2,0) + Cuu_0u_LNP*YuucL(2,1) + Cuu_uu_LNP*YuucL(0,0)*YuucL(2,1)).real();
972 Cuu_1231i_LNP = (Cuu_uu_LNP*YuucL(0,1)*YuucL(2,0) + Cuu_0u_LNP*YuucL(2,1) + Cuu_uu_LNP*YuucL(0,0)*YuucL(2,1)).imag();
973 Cuu_1232r_LNP = (2*Cuu_uu_LNP*YuucL(0,1)*YuucL(2,1)).real();
974 Cuu_1232i_LNP = (2*Cuu_uu_LNP*YuucL(0,1)*YuucL(2,1)).imag();
975 Cuu_1233r_LNP = (Cuu_u0_LNP*YuucL(0,1) + Cuu_uu_LNP*YuucL(0,2)*YuucL(2,1) + Cuu_uu_LNP*YuucL(0,1)*YuucL(2,2)).real();
976 Cuu_1233i_LNP = (Cuu_u0_LNP*YuucL(0,1) + Cuu_uu_LNP*YuucL(0,2)*YuucL(2,1) + Cuu_uu_LNP*YuucL(0,1)*YuucL(2,2)).imag();
977 Cuu_1313r_LNP = (2*Cuu_uu_LNP*YuucL(0,2)*YuucL(0,2)).real();
978 Cuu_1313i_LNP = (2*Cuu_uu_LNP*YuucL(0,2)*YuucL(0,2)).imag();
979 Cuu_1322r_LNP = (Cuu_u0_LNP*YuucL(0,2) + Cuu_uu_LNP*YuucL(0,2)*YuucL(1,1) + Cuu_uu_LNP*YuucL(0,1)*YuucL(1,2)).real();
980 Cuu_1322i_LNP = (Cuu_u0_LNP*YuucL(0,2) + Cuu_uu_LNP*YuucL(0,2)*YuucL(1,1) + Cuu_uu_LNP*YuucL(0,1)*YuucL(1,2)).imag();
981 Cuu_1323r_LNP = (2*Cuu_uu_LNP*YuucL(0,2)*YuucL(1,2)).real();
982 Cuu_1323i_LNP = (2*Cuu_uu_LNP*YuucL(0,2)*YuucL(1,2)).imag();
983 Cuu_1331r_LNP = (Cuu_00_LNP + Cuu_u0_LNP*YuucL(0,0) + Cuu_uu_LNP*YuucL(0,2)*YuucL(2,0) + Cuu_0u_LNP*YuucL(2,2) + Cuu_uu_LNP*YuucL(0,0)*YuucL(2,2)).real();
984 Cuu_1332r_LNP = (Cuu_u0_LNP*YuucL(0,1) + Cuu_uu_LNP*YuucL(0,2)*YuucL(2,1) + Cuu_uu_LNP*YuucL(0,1)*YuucL(2,2)).real();
985 Cuu_1332i_LNP = (Cuu_u0_LNP*YuucL(0,1) + Cuu_uu_LNP*YuucL(0,2)*YuucL(2,1) + Cuu_uu_LNP*YuucL(0,1)*YuucL(2,2)).imag();
986 Cuu_1333r_LNP = (2*Cuu_u0_LNP*YuucL(0,2) + 2*Cuu_uu_LNP*YuucL(0,2)*YuucL(2,2)).real();
987 Cuu_1333i_LNP = (2*Cuu_u0_LNP*YuucL(0,2) + 2*Cuu_uu_LNP*YuucL(0,2)*YuucL(2,2)).imag();
988 Cuu_2222r_LNP = (2*Cuu_00_LNP + 2*Cuu_0u_LNP*YuucL(1,1) + 2*Cuu_u0_LNP*YuucL(1,1) + 2*Cuu_uu_LNP*YuucL(1,1)*YuucL(1,1)).real();
989 Cuu_2223r_LNP = (Cuu_0u_LNP*YuucL(1,2) + Cuu_u0_LNP*YuucL(1,2) + 2*Cuu_uu_LNP*YuucL(1,1)*YuucL(1,2)).real();
990 Cuu_2223i_LNP = (Cuu_0u_LNP*YuucL(1,2) + Cuu_u0_LNP*YuucL(1,2) + 2*Cuu_uu_LNP*YuucL(1,1)*YuucL(1,2)).imag();
991 Cuu_2233r_LNP = (Cuu_00_LNP + Cuu_u0_LNP*YuucL(1,1) + Cuu_uu_LNP*YuucL(1,2)*YuucL(2,1) + Cuu_0u_LNP*YuucL(2,2) + Cuu_uu_LNP*YuucL(1,1)*YuucL(2,2)).real();
992 Cuu_2323r_LNP = (2*Cuu_uu_LNP*YuucL(1,2)*YuucL(1,2)).real();
993 Cuu_2323i_LNP = (2*Cuu_uu_LNP*YuucL(1,2)*YuucL(1,2)).imag();
994 Cuu_2332r_LNP = (Cuu_00_LNP + Cuu_u0_LNP*YuucL(1,1) + Cuu_uu_LNP*YuucL(1,2)*YuucL(2,1) + Cuu_0u_LNP*YuucL(2,2) + Cuu_uu_LNP*YuucL(1,1)*YuucL(2,2)).real();
995 Cuu_2333r_LNP = (2*Cuu_u0_LNP*YuucL(1,2) + 2*Cuu_uu_LNP*YuucL(1,2)*YuucL(2,2)).real();
996 Cuu_2333i_LNP = (2*Cuu_u0_LNP*YuucL(1,2) + 2*Cuu_uu_LNP*YuucL(1,2)*YuucL(2,2)).imag();
997 Cuu_3333r_LNP = (2*Cuu_00_LNP + 2*Cuu_0u_LNP*YuucL(2,2) + 2*Cuu_u0_LNP*YuucL(2,2) + 2*Cuu_uu_LNP*YuucL(2,2)*YuucL(2,2)).real();
998
999 Cdd_1111r_LNP = (2*Cdd_00_LNP + 2*Cdd_0d_LNP*YddL(0) + 2*Cdd_d0_LNP*YddL(0) + 2*Cdd_dd_LNP*YddL(0)*YddL(0)).real();
1000 Cdd_1122r_LNP = (Cdd_00_LNP + Cdd_d0_LNP*YddL(0) + Cdd_0d_LNP*YddL(1) + Cdd_dd_LNP*YddL(0)*YddL(1)).real();
1001 Cdd_1133r_LNP = (Cdd_00_LNP + Cdd_d0_LNP*YddL(0) + Cdd_0d_LNP*YddL(2) + Cdd_dd_LNP*YddL(0)*YddL(2)).real();
1002 Cdd_1221r_LNP = (Cdd_00_LNP + Cdd_d0_LNP*YddL(0) + Cdd_0d_LNP*YddL(1) + Cdd_dd_LNP*YddL(0)*YddL(1)).real();
1003 Cdd_1331r_LNP = (Cdd_00_LNP + Cdd_d0_LNP*YddL(0) + Cdd_0d_LNP*YddL(2) + Cdd_dd_LNP*YddL(0)*YddL(2)).real();
1004 Cdd_2222r_LNP = (2*Cdd_00_LNP + 2*Cdd_0d_LNP*YddL(1) + 2*Cdd_d0_LNP*YddL(1) + 2*Cdd_dd_LNP*YddL(1)*YddL(1)).real();
1005 Cdd_2233r_LNP = (Cdd_00_LNP + Cdd_d0_LNP*YddL(1) + Cdd_0d_LNP*YddL(2) + Cdd_dd_LNP*YddL(1)*YddL(2)).real();
1006 Cdd_2332r_LNP = (Cdd_00_LNP + Cdd_d0_LNP*YddL(1) + Cdd_0d_LNP*YddL(2) + Cdd_dd_LNP*YddL(1)*YddL(2)).real();
1007 Cdd_3333r_LNP = (2*Cdd_00_LNP + 2*Cdd_0d_LNP*YddL(2) + 2*Cdd_d0_LNP*YddL(2) + 2*Cdd_dd_LNP*YddL(2)*YddL(2)).real();
1008
1009 Cud1_1111r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*YddL(0) + Cud1_u0_LNP*YuucL(0,0) + Cud1_ud_LNP*YddL(0)*YuucL(0,0)).real();
1010 Cud1_1122r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*YddL(1) + Cud1_u0_LNP*YuucL(0,0) + Cud1_ud_LNP*YddL(1)*YuucL(0,0)).real();
1011 Cud1_1133r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*YddL(2) + Cud1_u0_LNP*YuucL(0,0) + Cud1_ud_LNP*YddL(2)*YuucL(0,0)).real();
1012 Cud1_1211r_LNP = (Cud1_u0_LNP*YuucL(0,1) + Cud1_ud_LNP*YddL(0)*YuucL(0,1)).real();
1013 Cud1_1211i_LNP = (Cud1_u0_LNP*YuucL(0,1) + Cud1_ud_LNP*YddL(0)*YuucL(0,1)).imag();
1014 Cud1_1222r_LNP = (Cud1_u0_LNP*YuucL(0,1) + Cud1_ud_LNP*YddL(1)*YuucL(0,1)).real();
1015 Cud1_1222i_LNP = (Cud1_u0_LNP*YuucL(0,1) + Cud1_ud_LNP*YddL(1)*YuucL(0,1)).imag();
1016 Cud1_1233r_LNP = (Cud1_u0_LNP*YuucL(0,1) + Cud1_ud_LNP*YddL(2)*YuucL(0,1)).real();
1017 Cud1_1233i_LNP = (Cud1_u0_LNP*YuucL(0,1) + Cud1_ud_LNP*YddL(2)*YuucL(0,1)).imag();
1018 Cud1_1311r_LNP = (Cud1_u0_LNP*YuucL(0,2) + Cud1_ud_LNP*YddL(0)*YuucL(0,2)).real();
1019 Cud1_1311i_LNP = (Cud1_u0_LNP*YuucL(0,2) + Cud1_ud_LNP*YddL(0)*YuucL(0,2)).imag();
1020 Cud1_1322r_LNP = (Cud1_u0_LNP*YuucL(0,2) + Cud1_ud_LNP*YddL(1)*YuucL(0,2)).real();
1021 Cud1_1322i_LNP = (Cud1_u0_LNP*YuucL(0,2) + Cud1_ud_LNP*YddL(1)*YuucL(0,2)).imag();
1022 Cud1_1333r_LNP = (Cud1_u0_LNP*YuucL(0,2) + Cud1_ud_LNP*YddL(2)*YuucL(0,2)).real();
1023 Cud1_1333i_LNP = (Cud1_u0_LNP*YuucL(0,2) + Cud1_ud_LNP*YddL(2)*YuucL(0,2)).imag();
1024 Cud1_2211r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*YddL(0) + Cud1_u0_LNP*YuucL(1,1) + Cud1_ud_LNP*YddL(0)*YuucL(1,1)).real();
1025 Cud1_2222r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*YddL(1) + Cud1_u0_LNP*YuucL(1,1) + Cud1_ud_LNP*YddL(1)*YuucL(1,1)).real();
1026 Cud1_2233r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*YddL(2) + Cud1_u0_LNP*YuucL(1,1) + Cud1_ud_LNP*YddL(2)*YuucL(1,1)).real();
1027 Cud1_2311r_LNP = (Cud1_u0_LNP*YuucL(1,2) + Cud1_ud_LNP*YddL(0)*YuucL(1,2)).real();
1028 Cud1_2311i_LNP = (Cud1_u0_LNP*YuucL(1,2) + Cud1_ud_LNP*YddL(0)*YuucL(1,2)).imag();
1029 Cud1_2322r_LNP = (Cud1_u0_LNP*YuucL(1,2) + Cud1_ud_LNP*YddL(1)*YuucL(1,2)).real();
1030 Cud1_2322i_LNP = (Cud1_u0_LNP*YuucL(1,2) + Cud1_ud_LNP*YddL(1)*YuucL(1,2)).imag();
1031 Cud1_2333r_LNP = (Cud1_u0_LNP*YuucL(1,2) + Cud1_ud_LNP*YddL(2)*YuucL(1,2)).real();
1032 Cud1_2333i_LNP = (Cud1_u0_LNP*YuucL(1,2) + Cud1_ud_LNP*YddL(2)*YuucL(1,2)).imag();
1033 Cud1_3311r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*YddL(0) + Cud1_u0_LNP*YuucL(2,2) + Cud1_ud_LNP*YddL(0)*YuucL(2,2)).real();
1034 Cud1_3322r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*YddL(1) + Cud1_u0_LNP*YuucL(2,2) + Cud1_ud_LNP*YddL(1)*YuucL(2,2)).real();
1035 Cud1_3333r_LNP = (Cud1_00_LNP + Cud1_0d_LNP*YddL(2) + Cud1_u0_LNP*YuucL(2,2) + Cud1_ud_LNP*YddL(2)*YuucL(2,2)).real();
1036
1037 Cud8_1111r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*YddL(0) + Cud8_u0_LNP*YuucL(0,0) + Cud8_ud_LNP*YddL(0)*YuucL(0,0)).real();
1038 Cud8_1122r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*YddL(1) + Cud8_u0_LNP*YuucL(0,0) + Cud8_ud_LNP*YddL(1)*YuucL(0,0)).real();
1039 Cud8_1133r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*YddL(2) + Cud8_u0_LNP*YuucL(0,0) + Cud8_ud_LNP*YddL(2)*YuucL(0,0)).real();
1040 Cud8_1211r_LNP = (Cud8_u0_LNP*YuucL(0,1) + Cud8_ud_LNP*YddL(0)*YuucL(0,1)).real();
1041 Cud8_1211i_LNP = (Cud8_u0_LNP*YuucL(0,1) + Cud8_ud_LNP*YddL(0)*YuucL(0,1)).imag();
1042 Cud8_1222r_LNP = (Cud8_u0_LNP*YuucL(0,1) + Cud8_ud_LNP*YddL(1)*YuucL(0,1)).real();
1043 Cud8_1222i_LNP = (Cud8_u0_LNP*YuucL(0,1) + Cud8_ud_LNP*YddL(1)*YuucL(0,1)).imag();
1044 Cud8_1233r_LNP = (Cud8_u0_LNP*YuucL(0,1) + Cud8_ud_LNP*YddL(2)*YuucL(0,1)).real();
1045 Cud8_1233i_LNP = (Cud8_u0_LNP*YuucL(0,1) + Cud8_ud_LNP*YddL(2)*YuucL(0,1)).imag();
1046 Cud8_1311r_LNP = (Cud8_u0_LNP*YuucL(0,2) + Cud8_ud_LNP*YddL(0)*YuucL(0,2)).real();
1047 Cud8_1311i_LNP = (Cud8_u0_LNP*YuucL(0,2) + Cud8_ud_LNP*YddL(0)*YuucL(0,2)).imag();
1048 Cud8_1322r_LNP = (Cud8_u0_LNP*YuucL(0,2) + Cud8_ud_LNP*YddL(1)*YuucL(0,2)).real();
1049 Cud8_1322i_LNP = (Cud8_u0_LNP*YuucL(0,2) + Cud8_ud_LNP*YddL(1)*YuucL(0,2)).imag();
1050 Cud8_1333r_LNP = (Cud8_u0_LNP*YuucL(0,2) + Cud8_ud_LNP*YddL(2)*YuucL(0,2)).real();
1051 Cud8_1333i_LNP = (Cud8_u0_LNP*YuucL(0,2) + Cud8_ud_LNP*YddL(2)*YuucL(0,2)).imag();
1052 Cud8_2211r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*YddL(0) + Cud8_u0_LNP*YuucL(1,1) + Cud8_ud_LNP*YddL(0)*YuucL(1,1)).real();
1053 Cud8_2222r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*YddL(1) + Cud8_u0_LNP*YuucL(1,1) + Cud8_ud_LNP*YddL(1)*YuucL(1,1)).real();
1054 Cud8_2233r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*YddL(2) + Cud8_u0_LNP*YuucL(1,1) + Cud8_ud_LNP*YddL(2)*YuucL(1,1)).real();
1055 Cud8_2311r_LNP = (Cud8_u0_LNP*YuucL(1,2) + Cud8_ud_LNP*YddL(0)*YuucL(1,2)).real();
1056 Cud8_2311i_LNP = (Cud8_u0_LNP*YuucL(1,2) + Cud8_ud_LNP*YddL(0)*YuucL(1,2)).imag();
1057 Cud8_2322r_LNP = (Cud8_u0_LNP*YuucL(1,2) + Cud8_ud_LNP*YddL(1)*YuucL(1,2)).real();
1058 Cud8_2322i_LNP = (Cud8_u0_LNP*YuucL(1,2) + Cud8_ud_LNP*YddL(1)*YuucL(1,2)).imag();
1059 Cud8_2333r_LNP = (Cud8_u0_LNP*YuucL(1,2) + Cud8_ud_LNP*YddL(2)*YuucL(1,2)).real();
1060 Cud8_2333i_LNP = (Cud8_u0_LNP*YuucL(1,2) + Cud8_ud_LNP*YddL(2)*YuucL(1,2)).imag();
1061 Cud8_3311r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*YddL(0) + Cud8_u0_LNP*YuucL(2,2) + Cud8_ud_LNP*YddL(0)*YuucL(2,2)).real();
1062 Cud8_3322r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*YddL(1) + Cud8_u0_LNP*YuucL(2,2) + Cud8_ud_LNP*YddL(1)*YuucL(2,2)).real();
1063 Cud8_3333r_LNP = (Cud8_00_LNP + Cud8_0d_LNP*YddL(2) + Cud8_u0_LNP*YuucL(2,2) + Cud8_ud_LNP*YddL(2)*YuucL(2,2)).real();
1064
1065 Cqu1_1111r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*YddL(0) + Cqu1_u0_LNP*YucuL(0,0) + Cqu1_0u_LNP*YuucL(0,0) + Cqu1_du_LNP*YddL(0)*YuucL(0,0) + Cqu1_uu_LNP*YucuL(0,0)*YuucL(0,0)).real();
1066 Cqu1_1112r_LNP = (Cqu1_0u_LNP*YuucL(0,1) + Cqu1_du_LNP*YddL(0)*YuucL(0,1) + Cqu1_uu_LNP*YucuL(0,0)*YuucL(0,1)).real();
1067 Cqu1_1112i_LNP = (Cqu1_0u_LNP*YuucL(0,1) + Cqu1_du_LNP*YddL(0)*YuucL(0,1) + Cqu1_uu_LNP*YucuL(0,0)*YuucL(0,1)).imag();
1068 Cqu1_1113r_LNP = (Cqu1_0u_LNP*YuucL(0,2) + Cqu1_du_LNP*YddL(0)*YuucL(0,2) + Cqu1_uu_LNP*YucuL(0,0)*YuucL(0,2)).real();
1069 Cqu1_1113i_LNP = (Cqu1_0u_LNP*YuucL(0,2) + Cqu1_du_LNP*YddL(0)*YuucL(0,2) + Cqu1_uu_LNP*YucuL(0,0)*YuucL(0,2)).imag();
1070 Cqu1_1122r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*YddL(0) + Cqu1_u0_LNP*YucuL(0,0) + Cqu1_0u_LNP*YuucL(1,1) + Cqu1_du_LNP*YddL(0)*YuucL(1,1) + Cqu1_uu_LNP*YucuL(0,0)*YuucL(1,1)).real();
1071 Cqu1_1123r_LNP = (Cqu1_0u_LNP*YuucL(1,2) + Cqu1_du_LNP*YddL(0)*YuucL(1,2) + Cqu1_uu_LNP*YucuL(0,0)*YuucL(1,2)).real();
1072 Cqu1_1123i_LNP = (Cqu1_0u_LNP*YuucL(1,2) + Cqu1_du_LNP*YddL(0)*YuucL(1,2) + Cqu1_uu_LNP*YucuL(0,0)*YuucL(1,2)).imag();
1073 Cqu1_1133r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*YddL(0) + Cqu1_u0_LNP*YucuL(0,0) + Cqu1_0u_LNP*YuucL(2,2) + Cqu1_du_LNP*YddL(0)*YuucL(2,2) + Cqu1_uu_LNP*YucuL(0,0)*YuucL(2,2)).real();
1074 Cqu1_1211r_LNP = (Cqu1_u0_LNP*YucuL(0,1) + Cqu1_uu_LNP*YucuL(0,1)*YuucL(0,0)).real();
1075 Cqu1_1211i_LNP = (Cqu1_u0_LNP*YucuL(0,1) + Cqu1_uu_LNP*YucuL(0,1)*YuucL(0,0)).imag();
1076 Cqu1_1212r_LNP = (Cqu1_uu_LNP*YucuL(0,1)*YuucL(0,1)).real();
1077 Cqu1_1212i_LNP = (Cqu1_uu_LNP*YucuL(0,1)*YuucL(0,1)).imag();
1078 Cqu1_1213r_LNP = (Cqu1_uu_LNP*YucuL(0,1)*YuucL(0,2)).real();
1079 Cqu1_1213i_LNP = (Cqu1_uu_LNP*YucuL(0,1)*YuucL(0,2)).imag();
1080 Cqu1_1221r_LNP = (Cqu1_uu_LNP*YucuL(0,1)*YuucL(1,0)).real();
1081 Cqu1_1221i_LNP = (Cqu1_uu_LNP*YucuL(0,1)*YuucL(1,0)).imag();
1082 Cqu1_1222r_LNP = (Cqu1_u0_LNP*YucuL(0,1) + Cqu1_uu_LNP*YucuL(0,1)*YuucL(1,1)).real();
1083 Cqu1_1222i_LNP = (Cqu1_u0_LNP*YucuL(0,1) + Cqu1_uu_LNP*YucuL(0,1)*YuucL(1,1)).imag();
1084 Cqu1_1223r_LNP = (Cqu1_uu_LNP*YucuL(0,1)*YuucL(1,2)).real();
1085 Cqu1_1223i_LNP = (Cqu1_uu_LNP*YucuL(0,1)*YuucL(1,2)).imag();
1086 Cqu1_1231r_LNP = (Cqu1_uu_LNP*YucuL(0,1)*YuucL(2,0)).real();
1087 Cqu1_1231i_LNP = (Cqu1_uu_LNP*YucuL(0,1)*YuucL(2,0)).imag();
1088 Cqu1_1232r_LNP = (Cqu1_uu_LNP*YucuL(0,1)*YuucL(2,1)).real();
1089 Cqu1_1232i_LNP = (Cqu1_uu_LNP*YucuL(0,1)*YuucL(2,1)).imag();
1090 Cqu1_1233r_LNP = (Cqu1_u0_LNP*YucuL(0,1) + Cqu1_uu_LNP*YucuL(0,1)*YuucL(2,2)).real();
1091 Cqu1_1233i_LNP = (Cqu1_u0_LNP*YucuL(0,1) + Cqu1_uu_LNP*YucuL(0,1)*YuucL(2,2)).imag();
1092 Cqu1_1311r_LNP = (Cqu1_u0_LNP*YucuL(0,2) + Cqu1_uu_LNP*YucuL(0,2)*YuucL(0,0)).real();
1093 Cqu1_1311i_LNP = (Cqu1_u0_LNP*YucuL(0,2) + Cqu1_uu_LNP*YucuL(0,2)*YuucL(0,0)).imag();
1094 Cqu1_1312r_LNP = (Cqu1_uu_LNP*YucuL(0,2)*YuucL(0,1)).real();
1095 Cqu1_1312i_LNP = (Cqu1_uu_LNP*YucuL(0,2)*YuucL(0,1)).imag();
1096 Cqu1_1313r_LNP = (Cqu1_uu_LNP*YucuL(0,2)*YuucL(0,2)).real();
1097 Cqu1_1313i_LNP = (Cqu1_uu_LNP*YucuL(0,2)*YuucL(0,2)).imag();
1098 Cqu1_1321r_LNP = (Cqu1_uu_LNP*YucuL(0,2)*YuucL(1,0)).real();
1099 Cqu1_1321i_LNP = (Cqu1_uu_LNP*YucuL(0,2)*YuucL(1,0)).imag();
1100 Cqu1_1322r_LNP = (Cqu1_u0_LNP*YucuL(0,2) + Cqu1_uu_LNP*YucuL(0,2)*YuucL(1,1)).real();
1101 Cqu1_1322i_LNP = (Cqu1_u0_LNP*YucuL(0,2) + Cqu1_uu_LNP*YucuL(0,2)*YuucL(1,1)).imag();
1102 Cqu1_1323r_LNP = (Cqu1_uu_LNP*YucuL(0,2)*YuucL(1,2)).real();
1103 Cqu1_1323i_LNP = (Cqu1_uu_LNP*YucuL(0,2)*YuucL(1,2)).imag();
1104 Cqu1_1331r_LNP = (Cqu1_uu_LNP*YucuL(0,2)*YuucL(2,0)).real();
1105 Cqu1_1331i_LNP = (Cqu1_uu_LNP*YucuL(0,2)*YuucL(2,0)).imag();
1106 Cqu1_1332r_LNP = (Cqu1_uu_LNP*YucuL(0,2)*YuucL(2,1)).real();
1107 Cqu1_1332i_LNP = (Cqu1_uu_LNP*YucuL(0,2)*YuucL(2,1)).imag();
1108 Cqu1_1333r_LNP = (Cqu1_u0_LNP*YucuL(0,2) + Cqu1_uu_LNP*YucuL(0,2)*YuucL(2,2)).real();
1109 Cqu1_1333i_LNP = (Cqu1_u0_LNP*YucuL(0,2) + Cqu1_uu_LNP*YucuL(0,2)*YuucL(2,2)).imag();
1110 Cqu1_2211r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*YddL(1) + Cqu1_u0_LNP*YucuL(1,1) + Cqu1_0u_LNP*YuucL(0,0) + Cqu1_du_LNP*YddL(1)*YuucL(0,0) + Cqu1_uu_LNP*YucuL(1,1)*YuucL(0,0)).real();
1111 Cqu1_2212r_LNP = (Cqu1_0u_LNP*YuucL(0,1) + Cqu1_du_LNP*YddL(1)*YuucL(0,1) + Cqu1_uu_LNP*YucuL(1,1)*YuucL(0,1)).real();
1112 Cqu1_2212i_LNP = (Cqu1_0u_LNP*YuucL(0,1) + Cqu1_du_LNP*YddL(1)*YuucL(0,1) + Cqu1_uu_LNP*YucuL(1,1)*YuucL(0,1)).imag();
1113 Cqu1_2213r_LNP = (Cqu1_0u_LNP*YuucL(0,2) + Cqu1_du_LNP*YddL(1)*YuucL(0,2) + Cqu1_uu_LNP*YucuL(1,1)*YuucL(0,2)).real();
1114 Cqu1_2213i_LNP = (Cqu1_0u_LNP*YuucL(0,2) + Cqu1_du_LNP*YddL(1)*YuucL(0,2) + Cqu1_uu_LNP*YucuL(1,1)*YuucL(0,2)).imag();
1115 Cqu1_2222r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*YddL(1) + Cqu1_u0_LNP*YucuL(1,1) + Cqu1_0u_LNP*YuucL(1,1) + Cqu1_du_LNP*YddL(1)*YuucL(1,1) + Cqu1_uu_LNP*YucuL(1,1)*YuucL(1,1)).real();
1116 Cqu1_2223r_LNP = (Cqu1_0u_LNP*YuucL(1,2) + Cqu1_du_LNP*YddL(1)*YuucL(1,2) + Cqu1_uu_LNP*YucuL(1,1)*YuucL(1,2)).real();
1117 Cqu1_2223i_LNP = (Cqu1_0u_LNP*YuucL(1,2) + Cqu1_du_LNP*YddL(1)*YuucL(1,2) + Cqu1_uu_LNP*YucuL(1,1)*YuucL(1,2)).imag();
1118 Cqu1_2233r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*YddL(1) + Cqu1_u0_LNP*YucuL(1,1) + Cqu1_0u_LNP*YuucL(2,2) + Cqu1_du_LNP*YddL(1)*YuucL(2,2) + Cqu1_uu_LNP*YucuL(1,1)*YuucL(2,2)).real();
1119 Cqu1_2311r_LNP = (Cqu1_u0_LNP*YucuL(1,2) + Cqu1_uu_LNP*YucuL(1,2)*YuucL(0,0)).real();
1120 Cqu1_2311i_LNP = (Cqu1_u0_LNP*YucuL(1,2) + Cqu1_uu_LNP*YucuL(1,2)*YuucL(0,0)).imag();
1121 Cqu1_2312r_LNP = (Cqu1_uu_LNP*YucuL(1,2)*YuucL(0,1)).real();
1122 Cqu1_2312i_LNP = (Cqu1_uu_LNP*YucuL(1,2)*YuucL(0,1)).imag();
1123 Cqu1_2313r_LNP = (Cqu1_uu_LNP*YucuL(1,2)*YuucL(0,2)).real();
1124 Cqu1_2313i_LNP = (Cqu1_uu_LNP*YucuL(1,2)*YuucL(0,2)).imag();
1125 Cqu1_2321r_LNP = (Cqu1_uu_LNP*YucuL(1,2)*YuucL(1,0)).real();
1126 Cqu1_2321i_LNP = (Cqu1_uu_LNP*YucuL(1,2)*YuucL(1,0)).imag();
1127 Cqu1_2322r_LNP = (Cqu1_u0_LNP*YucuL(1,2) + Cqu1_uu_LNP*YucuL(1,2)*YuucL(1,1)).real();
1128 Cqu1_2322i_LNP = (Cqu1_u0_LNP*YucuL(1,2) + Cqu1_uu_LNP*YucuL(1,2)*YuucL(1,1)).imag();
1129 Cqu1_2323r_LNP = (Cqu1_uu_LNP*YucuL(1,2)*YuucL(1,2)).real();
1130 Cqu1_2323i_LNP = (Cqu1_uu_LNP*YucuL(1,2)*YuucL(1,2)).imag();
1131 Cqu1_2331r_LNP = (Cqu1_uu_LNP*YucuL(1,2)*YuucL(2,0)).real();
1132 Cqu1_2331i_LNP = (Cqu1_uu_LNP*YucuL(1,2)*YuucL(2,0)).imag();
1133 Cqu1_2332r_LNP = (Cqu1_uu_LNP*YucuL(1,2)*YuucL(2,1)).real();
1134 Cqu1_2332i_LNP = (Cqu1_uu_LNP*YucuL(1,2)*YuucL(2,1)).imag();
1135 Cqu1_2333r_LNP = (Cqu1_u0_LNP*YucuL(1,2) + Cqu1_uu_LNP*YucuL(1,2)*YuucL(2,2)).real();
1136 Cqu1_2333i_LNP = (Cqu1_u0_LNP*YucuL(1,2) + Cqu1_uu_LNP*YucuL(1,2)*YuucL(2,2)).imag();
1137 Cqu1_3311r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*YddL(2) + Cqu1_u0_LNP*YucuL(2,2) + Cqu1_0u_LNP*YuucL(0,0) + Cqu1_du_LNP*YddL(2)*YuucL(0,0) + Cqu1_uu_LNP*YucuL(2,2)*YuucL(0,0)).real();
1138 Cqu1_3312r_LNP = (Cqu1_0u_LNP*YuucL(0,1) + Cqu1_du_LNP*YddL(2)*YuucL(0,1) + Cqu1_uu_LNP*YucuL(2,2)*YuucL(0,1)).real();
1139 Cqu1_3312i_LNP = (Cqu1_0u_LNP*YuucL(0,1) + Cqu1_du_LNP*YddL(2)*YuucL(0,1) + Cqu1_uu_LNP*YucuL(2,2)*YuucL(0,1)).imag();
1140 Cqu1_3313r_LNP = (Cqu1_0u_LNP*YuucL(0,2) + Cqu1_du_LNP*YddL(2)*YuucL(0,2) + Cqu1_uu_LNP*YucuL(2,2)*YuucL(0,2)).real();
1141 Cqu1_3313i_LNP = (Cqu1_0u_LNP*YuucL(0,2) + Cqu1_du_LNP*YddL(2)*YuucL(0,2) + Cqu1_uu_LNP*YucuL(2,2)*YuucL(0,2)).imag();
1142 Cqu1_3322r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*YddL(2) + Cqu1_u0_LNP*YucuL(2,2) + Cqu1_0u_LNP*YuucL(1,1) + Cqu1_du_LNP*YddL(2)*YuucL(1,1) + Cqu1_uu_LNP*YucuL(2,2)*YuucL(1,1)).real();
1143 Cqu1_3323r_LNP = (Cqu1_0u_LNP*YuucL(1,2) + Cqu1_du_LNP*YddL(2)*YuucL(1,2) + Cqu1_uu_LNP*YucuL(2,2)*YuucL(1,2)).real();
1144 Cqu1_3323i_LNP = (Cqu1_0u_LNP*YuucL(1,2) + Cqu1_du_LNP*YddL(2)*YuucL(1,2) + Cqu1_uu_LNP*YucuL(2,2)*YuucL(1,2)).imag();
1145 Cqu1_3333r_LNP = (Cqu1_00_LNP + Cqu1_d0_LNP*YddL(2) + Cqu1_u0_LNP*YucuL(2,2) + Cqu1_0u_LNP*YuucL(2,2) + Cqu1_du_LNP*YddL(2)*YuucL(2,2) + Cqu1_uu_LNP*YucuL(2,2)*YuucL(2,2)).real();
1146
1147 Cqu8_1111r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*YddL(0) + Cqu8_u0_LNP*YucuL(0,0) + Cqu8_0u_LNP*YuucL(0,0) + Cqu8_du_LNP*YddL(0)*YuucL(0,0) + Cqu8_uu_LNP*YucuL(0,0)*YuucL(0,0)).real();
1148 Cqu8_1112r_LNP = (Cqu8_0u_LNP*YuucL(0,1) + Cqu8_du_LNP*YddL(0)*YuucL(0,1) + Cqu8_uu_LNP*YucuL(0,0)*YuucL(0,1)).real();
1149 Cqu8_1112i_LNP = (Cqu8_0u_LNP*YuucL(0,1) + Cqu8_du_LNP*YddL(0)*YuucL(0,1) + Cqu8_uu_LNP*YucuL(0,0)*YuucL(0,1)).imag();
1150 Cqu8_1113r_LNP = (Cqu8_0u_LNP*YuucL(0,2) + Cqu8_du_LNP*YddL(0)*YuucL(0,2) + Cqu8_uu_LNP*YucuL(0,0)*YuucL(0,2)).real();
1151 Cqu8_1113i_LNP = (Cqu8_0u_LNP*YuucL(0,2) + Cqu8_du_LNP*YddL(0)*YuucL(0,2) + Cqu8_uu_LNP*YucuL(0,0)*YuucL(0,2)).imag();
1152 Cqu8_1122r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*YddL(0) + Cqu8_u0_LNP*YucuL(0,0) + Cqu8_0u_LNP*YuucL(1,1) + Cqu8_du_LNP*YddL(0)*YuucL(1,1) + Cqu8_uu_LNP*YucuL(0,0)*YuucL(1,1)).real();
1153 Cqu8_1123r_LNP = (Cqu8_0u_LNP*YuucL(1,2) + Cqu8_du_LNP*YddL(0)*YuucL(1,2) + Cqu8_uu_LNP*YucuL(0,0)*YuucL(1,2)).real();
1154 Cqu8_1123i_LNP = (Cqu8_0u_LNP*YuucL(1,2) + Cqu8_du_LNP*YddL(0)*YuucL(1,2) + Cqu8_uu_LNP*YucuL(0,0)*YuucL(1,2)).imag();
1155 Cqu8_1133r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*YddL(0) + Cqu8_u0_LNP*YucuL(0,0) + Cqu8_0u_LNP*YuucL(2,2) + Cqu8_du_LNP*YddL(0)*YuucL(2,2) + Cqu8_uu_LNP*YucuL(0,0)*YuucL(2,2)).real();
1156 Cqu8_1211r_LNP = (Cqu8_u0_LNP*YucuL(0,1) + Cqu8_uu_LNP*YucuL(0,1)*YuucL(0,0)).real();
1157 Cqu8_1211i_LNP = (Cqu8_u0_LNP*YucuL(0,1) + Cqu8_uu_LNP*YucuL(0,1)*YuucL(0,0)).imag();
1158 Cqu8_1212r_LNP = (Cqu8_uu_LNP*YucuL(0,1)*YuucL(0,1)).real();
1159 Cqu8_1212i_LNP = (Cqu8_uu_LNP*YucuL(0,1)*YuucL(0,1)).imag();
1160 Cqu8_1213r_LNP = (Cqu8_uu_LNP*YucuL(0,1)*YuucL(0,2)).real();
1161 Cqu8_1213i_LNP = (Cqu8_uu_LNP*YucuL(0,1)*YuucL(0,2)).imag();
1162 Cqu8_1221r_LNP = (Cqu8_uu_LNP*YucuL(0,1)*YuucL(1,0)).real();
1163 Cqu8_1221i_LNP = (Cqu8_uu_LNP*YucuL(0,1)*YuucL(1,0)).imag();
1164 Cqu8_1222r_LNP = (Cqu8_u0_LNP*YucuL(0,1) + Cqu8_uu_LNP*YucuL(0,1)*YuucL(1,1)).real();
1165 Cqu8_1222i_LNP = (Cqu8_u0_LNP*YucuL(0,1) + Cqu8_uu_LNP*YucuL(0,1)*YuucL(1,1)).imag();
1166 Cqu8_1223r_LNP = (Cqu8_uu_LNP*YucuL(0,1)*YuucL(1,2)).real();
1167 Cqu8_1223i_LNP = (Cqu8_uu_LNP*YucuL(0,1)*YuucL(1,2)).imag();
1168 Cqu8_1231r_LNP = (Cqu8_uu_LNP*YucuL(0,1)*YuucL(2,0)).real();
1169 Cqu8_1231i_LNP = (Cqu8_uu_LNP*YucuL(0,1)*YuucL(2,0)).imag();
1170 Cqu8_1232r_LNP = (Cqu8_uu_LNP*YucuL(0,1)*YuucL(2,1)).real();
1171 Cqu8_1232i_LNP = (Cqu8_uu_LNP*YucuL(0,1)*YuucL(2,1)).imag();
1172 Cqu8_1233r_LNP = (Cqu8_u0_LNP*YucuL(0,1) + Cqu8_uu_LNP*YucuL(0,1)*YuucL(2,2)).real();
1173 Cqu8_1233i_LNP = (Cqu8_u0_LNP*YucuL(0,1) + Cqu8_uu_LNP*YucuL(0,1)*YuucL(2,2)).imag();
1174 Cqu8_1311r_LNP = (Cqu8_u0_LNP*YucuL(0,2) + Cqu8_uu_LNP*YucuL(0,2)*YuucL(0,0)).real();
1175 Cqu8_1311i_LNP = (Cqu8_u0_LNP*YucuL(0,2) + Cqu8_uu_LNP*YucuL(0,2)*YuucL(0,0)).imag();
1176 Cqu8_1312r_LNP = (Cqu8_uu_LNP*YucuL(0,2)*YuucL(0,1)).real();
1177 Cqu8_1312i_LNP = (Cqu8_uu_LNP*YucuL(0,2)*YuucL(0,1)).imag();
1178 Cqu8_1313r_LNP = (Cqu8_uu_LNP*YucuL(0,2)*YuucL(0,2)).real();
1179 Cqu8_1313i_LNP = (Cqu8_uu_LNP*YucuL(0,2)*YuucL(0,2)).imag();
1180 Cqu8_1321r_LNP = (Cqu8_uu_LNP*YucuL(0,2)*YuucL(1,0)).real();
1181 Cqu8_1321i_LNP = (Cqu8_uu_LNP*YucuL(0,2)*YuucL(1,0)).imag();
1182 Cqu8_1322r_LNP = (Cqu8_u0_LNP*YucuL(0,2) + Cqu8_uu_LNP*YucuL(0,2)*YuucL(1,1)).real();
1183 Cqu8_1322i_LNP = (Cqu8_u0_LNP*YucuL(0,2) + Cqu8_uu_LNP*YucuL(0,2)*YuucL(1,1)).imag();
1184 Cqu8_1323r_LNP = (Cqu8_uu_LNP*YucuL(0,2)*YuucL(1,2)).real();
1185 Cqu8_1323i_LNP = (Cqu8_uu_LNP*YucuL(0,2)*YuucL(1,2)).imag();
1186 Cqu8_1331r_LNP = (Cqu8_uu_LNP*YucuL(0,2)*YuucL(2,0)).real();
1187 Cqu8_1331i_LNP = (Cqu8_uu_LNP*YucuL(0,2)*YuucL(2,0)).imag();
1188 Cqu8_1332r_LNP = (Cqu8_uu_LNP*YucuL(0,2)*YuucL(2,1)).real();
1189 Cqu8_1332i_LNP = (Cqu8_uu_LNP*YucuL(0,2)*YuucL(2,1)).imag();
1190 Cqu8_1333r_LNP = (Cqu8_u0_LNP*YucuL(0,2) + Cqu8_uu_LNP*YucuL(0,2)*YuucL(2,2)).real();
1191 Cqu8_1333i_LNP = (Cqu8_u0_LNP*YucuL(0,2) + Cqu8_uu_LNP*YucuL(0,2)*YuucL(2,2)).imag();
1192 Cqu8_2211r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*YddL(1) + Cqu8_u0_LNP*YucuL(1,1) + Cqu8_0u_LNP*YuucL(0,0) + Cqu8_du_LNP*YddL(1)*YuucL(0,0) + Cqu8_uu_LNP*YucuL(1,1)*YuucL(0,0)).real();
1193 Cqu8_2212r_LNP = (Cqu8_0u_LNP*YuucL(0,1) + Cqu8_du_LNP*YddL(1)*YuucL(0,1) + Cqu8_uu_LNP*YucuL(1,1)*YuucL(0,1)).real();
1194 Cqu8_2212i_LNP = (Cqu8_0u_LNP*YuucL(0,1) + Cqu8_du_LNP*YddL(1)*YuucL(0,1) + Cqu8_uu_LNP*YucuL(1,1)*YuucL(0,1)).imag();
1195 Cqu8_2213r_LNP = (Cqu8_0u_LNP*YuucL(0,2) + Cqu8_du_LNP*YddL(1)*YuucL(0,2) + Cqu8_uu_LNP*YucuL(1,1)*YuucL(0,2)).real();
1196 Cqu8_2213i_LNP = (Cqu8_0u_LNP*YuucL(0,2) + Cqu8_du_LNP*YddL(1)*YuucL(0,2) + Cqu8_uu_LNP*YucuL(1,1)*YuucL(0,2)).imag();
1197 Cqu8_2222r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*YddL(1) + Cqu8_u0_LNP*YucuL(1,1) + Cqu8_0u_LNP*YuucL(1,1) + Cqu8_du_LNP*YddL(1)*YuucL(1,1) + Cqu8_uu_LNP*YucuL(1,1)*YuucL(1,1)).real();
1198 Cqu8_2223r_LNP = (Cqu8_0u_LNP*YuucL(1,2) + Cqu8_du_LNP*YddL(1)*YuucL(1,2) + Cqu8_uu_LNP*YucuL(1,1)*YuucL(1,2)).real();
1199 Cqu8_2223i_LNP = (Cqu8_0u_LNP*YuucL(1,2) + Cqu8_du_LNP*YddL(1)*YuucL(1,2) + Cqu8_uu_LNP*YucuL(1,1)*YuucL(1,2)).imag();
1200 Cqu8_2233r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*YddL(1) + Cqu8_u0_LNP*YucuL(1,1) + Cqu8_0u_LNP*YuucL(2,2) + Cqu8_du_LNP*YddL(1)*YuucL(2,2) + Cqu8_uu_LNP*YucuL(1,1)*YuucL(2,2)).real();
1201 Cqu8_2311r_LNP = (Cqu8_u0_LNP*YucuL(1,2) + Cqu8_uu_LNP*YucuL(1,2)*YuucL(0,0)).real();
1202 Cqu8_2311i_LNP = (Cqu8_u0_LNP*YucuL(1,2) + Cqu8_uu_LNP*YucuL(1,2)*YuucL(0,0)).imag();
1203 Cqu8_2312r_LNP = (Cqu8_uu_LNP*YucuL(1,2)*YuucL(0,1)).real();
1204 Cqu8_2312i_LNP = (Cqu8_uu_LNP*YucuL(1,2)*YuucL(0,1)).imag();
1205 Cqu8_2313r_LNP = (Cqu8_uu_LNP*YucuL(1,2)*YuucL(0,2)).real();
1206 Cqu8_2313i_LNP = (Cqu8_uu_LNP*YucuL(1,2)*YuucL(0,2)).imag();
1207 Cqu8_2321r_LNP = (Cqu8_uu_LNP*YucuL(1,2)*YuucL(1,0)).real();
1208 Cqu8_2321i_LNP = (Cqu8_uu_LNP*YucuL(1,2)*YuucL(1,0)).imag();
1209 Cqu8_2322r_LNP = (Cqu8_u0_LNP*YucuL(1,2) + Cqu8_uu_LNP*YucuL(1,2)*YuucL(1,1)).real();
1210 Cqu8_2322i_LNP = (Cqu8_u0_LNP*YucuL(1,2) + Cqu8_uu_LNP*YucuL(1,2)*YuucL(1,1)).imag();
1211 Cqu8_2323r_LNP = (Cqu8_uu_LNP*YucuL(1,2)*YuucL(1,2)).real();
1212 Cqu8_2323i_LNP = (Cqu8_uu_LNP*YucuL(1,2)*YuucL(1,2)).imag();
1213 Cqu8_2331r_LNP = (Cqu8_uu_LNP*YucuL(1,2)*YuucL(2,0)).real();
1214 Cqu8_2331i_LNP = (Cqu8_uu_LNP*YucuL(1,2)*YuucL(2,0)).imag();
1215 Cqu8_2332r_LNP = (Cqu8_uu_LNP*YucuL(1,2)*YuucL(2,1)).real();
1216 Cqu8_2332i_LNP = (Cqu8_uu_LNP*YucuL(1,2)*YuucL(2,1)).imag();
1217 Cqu8_2333r_LNP = (Cqu8_u0_LNP*YucuL(1,2) + Cqu8_uu_LNP*YucuL(1,2)*YuucL(2,2)).real();
1218 Cqu8_2333i_LNP = (Cqu8_u0_LNP*YucuL(1,2) + Cqu8_uu_LNP*YucuL(1,2)*YuucL(2,2)).imag();
1219 Cqu8_3311r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*YddL(2) + Cqu8_u0_LNP*YucuL(2,2) + Cqu8_0u_LNP*YuucL(0,0) + Cqu8_du_LNP*YddL(2)*YuucL(0,0) + Cqu8_uu_LNP*YucuL(2,2)*YuucL(0,0)).real();
1220 Cqu8_3312r_LNP = (Cqu8_0u_LNP*YuucL(0,1) + Cqu8_du_LNP*YddL(2)*YuucL(0,1) + Cqu8_uu_LNP*YucuL(2,2)*YuucL(0,1)).real();
1221 Cqu8_3312i_LNP = (Cqu8_0u_LNP*YuucL(0,1) + Cqu8_du_LNP*YddL(2)*YuucL(0,1) + Cqu8_uu_LNP*YucuL(2,2)*YuucL(0,1)).imag();
1222 Cqu8_3313r_LNP = (Cqu8_0u_LNP*YuucL(0,2) + Cqu8_du_LNP*YddL(2)*YuucL(0,2) + Cqu8_uu_LNP*YucuL(2,2)*YuucL(0,2)).real();
1223 Cqu8_3313i_LNP = (Cqu8_0u_LNP*YuucL(0,2) + Cqu8_du_LNP*YddL(2)*YuucL(0,2) + Cqu8_uu_LNP*YucuL(2,2)*YuucL(0,2)).imag();
1224 Cqu8_3322r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*YddL(2) + Cqu8_u0_LNP*YucuL(2,2) + Cqu8_0u_LNP*YuucL(1,1) + Cqu8_du_LNP*YddL(2)*YuucL(1,1) + Cqu8_uu_LNP*YucuL(2,2)*YuucL(1,1)).real();
1225 Cqu8_3323r_LNP = (Cqu8_0u_LNP*YuucL(1,2) + Cqu8_du_LNP*YddL(2)*YuucL(1,2) + Cqu8_uu_LNP*YucuL(2,2)*YuucL(1,2)).real();
1226 Cqu8_3323i_LNP = (Cqu8_0u_LNP*YuucL(1,2) + Cqu8_du_LNP*YddL(2)*YuucL(1,2) + Cqu8_uu_LNP*YucuL(2,2)*YuucL(1,2)).imag();
1227 Cqu8_3333r_LNP = (Cqu8_00_LNP + Cqu8_d0_LNP*YddL(2) + Cqu8_u0_LNP*YucuL(2,2) + Cqu8_0u_LNP*YuucL(2,2) + Cqu8_du_LNP*YddL(2)*YuucL(2,2) + Cqu8_uu_LNP*YucuL(2,2)*YuucL(2,2)).real();
1228
1229 Cqd1_1111r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*YddL(0) + Cqd1_d0_LNP*YddL(0) + Cqd1_dd_LNP*YddL(0)*YddL(0) + Cqd1_u0_LNP*YucuL(0,0) + Cqd1_ud_LNP*YddL(0)*YucuL(0,0)).real();
1230 Cqd1_1122r_LNP = (Cqd1_00_LNP + Cqd1_d0_LNP*YddL(0) + Cqd1_0d_LNP*YddL(1) + Cqd1_dd_LNP*YddL(0)*YddL(1) + Cqd1_u0_LNP*YucuL(0,0) + Cqd1_ud_LNP*YddL(1)*YucuL(0,0)).real();
1231 Cqd1_1133r_LNP = (Cqd1_00_LNP + Cqd1_d0_LNP*YddL(0) + Cqd1_0d_LNP*YddL(2) + Cqd1_dd_LNP*YddL(0)*YddL(2) + Cqd1_u0_LNP*YucuL(0,0) + Cqd1_ud_LNP*YddL(2)*YucuL(0,0)).real();
1232 Cqd1_1211r_LNP = (Cqd1_u0_LNP*YucuL(0,1) + Cqd1_ud_LNP*YddL(0)*YucuL(0,1)).real();
1233 Cqd1_1211i_LNP = (Cqd1_u0_LNP*YucuL(0,1) + Cqd1_ud_LNP*YddL(0)*YucuL(0,1)).imag();
1234 Cqd1_1222r_LNP = (Cqd1_u0_LNP*YucuL(0,1) + Cqd1_ud_LNP*YddL(1)*YucuL(0,1)).real();
1235 Cqd1_1222i_LNP = (Cqd1_u0_LNP*YucuL(0,1) + Cqd1_ud_LNP*YddL(1)*YucuL(0,1)).imag();
1236 Cqd1_1233r_LNP = (Cqd1_u0_LNP*YucuL(0,1) + Cqd1_ud_LNP*YddL(2)*YucuL(0,1)).real();
1237 Cqd1_1233i_LNP = (Cqd1_u0_LNP*YucuL(0,1) + Cqd1_ud_LNP*YddL(2)*YucuL(0,1)).imag();
1238 Cqd1_1311r_LNP = (Cqd1_u0_LNP*YucuL(0,2) + Cqd1_ud_LNP*YddL(0)*YucuL(0,2)).real();
1239 Cqd1_1311i_LNP = (Cqd1_u0_LNP*YucuL(0,2) + Cqd1_ud_LNP*YddL(0)*YucuL(0,2)).imag();
1240 Cqd1_1322r_LNP = (Cqd1_u0_LNP*YucuL(0,2) + Cqd1_ud_LNP*YddL(1)*YucuL(0,2)).real();
1241 Cqd1_1322i_LNP = (Cqd1_u0_LNP*YucuL(0,2) + Cqd1_ud_LNP*YddL(1)*YucuL(0,2)).imag();
1242 Cqd1_1333r_LNP = (Cqd1_u0_LNP*YucuL(0,2) + Cqd1_ud_LNP*YddL(2)*YucuL(0,2)).real();
1243 Cqd1_1333i_LNP = (Cqd1_u0_LNP*YucuL(0,2) + Cqd1_ud_LNP*YddL(2)*YucuL(0,2)).imag();
1244 Cqd1_2211r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*YddL(0) + Cqd1_d0_LNP*YddL(1) + Cqd1_dd_LNP*YddL(0)*YddL(1) + Cqd1_u0_LNP*YucuL(1,1) + Cqd1_ud_LNP*YddL(0)*YucuL(1,1)).real();
1245 Cqd1_2222r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*YddL(1) + Cqd1_d0_LNP*YddL(1) + Cqd1_dd_LNP*YddL(1)*YddL(1) + Cqd1_u0_LNP*YucuL(1,1) + Cqd1_ud_LNP*YddL(1)*YucuL(1,1)).real();
1246 Cqd1_2233r_LNP = (Cqd1_00_LNP + Cqd1_d0_LNP*YddL(1) + Cqd1_0d_LNP*YddL(2) + Cqd1_dd_LNP*YddL(1)*YddL(2) + Cqd1_u0_LNP*YucuL(1,1) + Cqd1_ud_LNP*YddL(2)*YucuL(1,1)).real();
1247 Cqd1_2311r_LNP = (Cqd1_u0_LNP*YucuL(1,2) + Cqd1_ud_LNP*YddL(0)*YucuL(1,2)).real();
1248 Cqd1_2311i_LNP = (Cqd1_u0_LNP*YucuL(1,2) + Cqd1_ud_LNP*YddL(0)*YucuL(1,2)).imag();
1249 Cqd1_2322r_LNP = (Cqd1_u0_LNP*YucuL(1,2) + Cqd1_ud_LNP*YddL(1)*YucuL(1,2)).real();
1250 Cqd1_2322i_LNP = (Cqd1_u0_LNP*YucuL(1,2) + Cqd1_ud_LNP*YddL(1)*YucuL(1,2)).imag();
1251 Cqd1_2333r_LNP = (Cqd1_u0_LNP*YucuL(1,2) + Cqd1_ud_LNP*YddL(2)*YucuL(1,2)).real();
1252 Cqd1_2333i_LNP = (Cqd1_u0_LNP*YucuL(1,2) + Cqd1_ud_LNP*YddL(2)*YucuL(1,2)).imag();
1253 Cqd1_3311r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*YddL(0) + Cqd1_d0_LNP*YddL(2) + Cqd1_dd_LNP*YddL(0)*YddL(2) + Cqd1_u0_LNP*YucuL(2,2) + Cqd1_ud_LNP*YddL(0)*YucuL(2,2)).real();
1254 Cqd1_3322r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*YddL(1) + Cqd1_d0_LNP*YddL(2) + Cqd1_dd_LNP*YddL(1)*YddL(2) + Cqd1_u0_LNP*YucuL(2,2) + Cqd1_ud_LNP*YddL(1)*YucuL(2,2)).real();
1255 Cqd1_3333r_LNP = (Cqd1_00_LNP + Cqd1_0d_LNP*YddL(2) + Cqd1_d0_LNP*YddL(2) + Cqd1_dd_LNP*YddL(2)*YddL(2) + Cqd1_u0_LNP*YucuL(2,2) + Cqd1_ud_LNP*YddL(2)*YucuL(2,2)).real();
1256
1257 Cqd8_1111r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*YddL(0) + Cqd8_d0_LNP*YddL(0) + Cqd8_dd_LNP*YddL(0)*YddL(0) + Cqd8_u0_LNP*YucuL(0,0) + Cqd8_ud_LNP*YddL(0)*YucuL(0,0)).real();
1258 Cqd8_1122r_LNP = (Cqd8_00_LNP + Cqd8_d0_LNP*YddL(0) + Cqd8_0d_LNP*YddL(1) + Cqd8_dd_LNP*YddL(0)*YddL(1) + Cqd8_u0_LNP*YucuL(0,0) + Cqd8_ud_LNP*YddL(1)*YucuL(0,0)).real();
1259 Cqd8_1133r_LNP = (Cqd8_00_LNP + Cqd8_d0_LNP*YddL(0) + Cqd8_0d_LNP*YddL(2) + Cqd8_dd_LNP*YddL(0)*YddL(2) + Cqd8_u0_LNP*YucuL(0,0) + Cqd8_ud_LNP*YddL(2)*YucuL(0,0)).real();
1260 Cqd8_1211r_LNP = (Cqd8_u0_LNP*YucuL(0,1) + Cqd8_ud_LNP*YddL(0)*YucuL(0,1)).real();
1261 Cqd8_1211i_LNP = (Cqd8_u0_LNP*YucuL(0,1) + Cqd8_ud_LNP*YddL(0)*YucuL(0,1)).imag();
1262 Cqd8_1222r_LNP = (Cqd8_u0_LNP*YucuL(0,1) + Cqd8_ud_LNP*YddL(1)*YucuL(0,1)).real();
1263 Cqd8_1222i_LNP = (Cqd8_u0_LNP*YucuL(0,1) + Cqd8_ud_LNP*YddL(1)*YucuL(0,1)).imag();
1264 Cqd8_1233r_LNP = (Cqd8_u0_LNP*YucuL(0,1) + Cqd8_ud_LNP*YddL(2)*YucuL(0,1)).real();
1265 Cqd8_1233i_LNP = (Cqd8_u0_LNP*YucuL(0,1) + Cqd8_ud_LNP*YddL(2)*YucuL(0,1)).imag();
1266 Cqd8_1311r_LNP = (Cqd8_u0_LNP*YucuL(0,2) + Cqd8_ud_LNP*YddL(0)*YucuL(0,2)).real();
1267 Cqd8_1311i_LNP = (Cqd8_u0_LNP*YucuL(0,2) + Cqd8_ud_LNP*YddL(0)*YucuL(0,2)).imag();
1268 Cqd8_1322r_LNP = (Cqd8_u0_LNP*YucuL(0,2) + Cqd8_ud_LNP*YddL(1)*YucuL(0,2)).real();
1269 Cqd8_1322i_LNP = (Cqd8_u0_LNP*YucuL(0,2) + Cqd8_ud_LNP*YddL(1)*YucuL(0,2)).imag();
1270 Cqd8_1333r_LNP = (Cqd8_u0_LNP*YucuL(0,2) + Cqd8_ud_LNP*YddL(2)*YucuL(0,2)).real();
1271 Cqd8_1333i_LNP = (Cqd8_u0_LNP*YucuL(0,2) + Cqd8_ud_LNP*YddL(2)*YucuL(0,2)).imag();
1272 Cqd8_2211r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*YddL(0) + Cqd8_d0_LNP*YddL(1) + Cqd8_dd_LNP*YddL(0)*YddL(1) + Cqd8_u0_LNP*YucuL(1,1) + Cqd8_ud_LNP*YddL(0)*YucuL(1,1)).real();
1273 Cqd8_2222r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*YddL(1) + Cqd8_d0_LNP*YddL(1) + Cqd8_dd_LNP*YddL(1)*YddL(1) + Cqd8_u0_LNP*YucuL(1,1) + Cqd8_ud_LNP*YddL(1)*YucuL(1,1)).real();
1274 Cqd8_2233r_LNP = (Cqd8_00_LNP + Cqd8_d0_LNP*YddL(1) + Cqd8_0d_LNP*YddL(2) + Cqd8_dd_LNP*YddL(1)*YddL(2) + Cqd8_u0_LNP*YucuL(1,1) + Cqd8_ud_LNP*YddL(2)*YucuL(1,1)).real();
1275 Cqd8_2311r_LNP = (Cqd8_u0_LNP*YucuL(1,2) + Cqd8_ud_LNP*YddL(0)*YucuL(1,2)).real();
1276 Cqd8_2311i_LNP = (Cqd8_u0_LNP*YucuL(1,2) + Cqd8_ud_LNP*YddL(0)*YucuL(1,2)).imag();
1277 Cqd8_2322r_LNP = (Cqd8_u0_LNP*YucuL(1,2) + Cqd8_ud_LNP*YddL(1)*YucuL(1,2)).real();
1278 Cqd8_2322i_LNP = (Cqd8_u0_LNP*YucuL(1,2) + Cqd8_ud_LNP*YddL(1)*YucuL(1,2)).imag();
1279 Cqd8_2333r_LNP = (Cqd8_u0_LNP*YucuL(1,2) + Cqd8_ud_LNP*YddL(2)*YucuL(1,2)).real();
1280 Cqd8_2333i_LNP = (Cqd8_u0_LNP*YucuL(1,2) + Cqd8_ud_LNP*YddL(2)*YucuL(1,2)).imag();
1281 Cqd8_3311r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*YddL(0) + Cqd8_d0_LNP*YddL(2) + Cqd8_dd_LNP*YddL(0)*YddL(2) + Cqd8_u0_LNP*YucuL(2,2) + Cqd8_ud_LNP*YddL(0)*YucuL(2,2)).real();
1282 Cqd8_3322r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*YddL(1) + Cqd8_d0_LNP*YddL(2) + Cqd8_dd_LNP*YddL(1)*YddL(2) + Cqd8_u0_LNP*YucuL(2,2) + Cqd8_ud_LNP*YddL(1)*YucuL(2,2)).real();
1283 Cqd8_3333r_LNP = (Cqd8_00_LNP + Cqd8_0d_LNP*YddL(2) + Cqd8_d0_LNP*YddL(2) + Cqd8_dd_LNP*YddL(2)*YddL(2) + Cqd8_u0_LNP*YucuL(2,2) + Cqd8_ud_LNP*YddL(2)*YucuL(2,2)).real();
1284
1285 Cquqd1_1111r_LNP = (2*Cquqd1_00_LNP*YdL(0)*YuL(0,0)).real();
1286 Cquqd1_1111i_LNP = (2*Cquqd1_00_LNP*YdL(0)*YuL(0,0)).imag();
1287 Cquqd1_1121r_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(1,0)).real();
1288 Cquqd1_1121i_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(1,0)).imag();
1289 Cquqd1_1122r_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(0,0)).real();
1290 Cquqd1_1122i_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(0,0)).imag();
1291 Cquqd1_1131r_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(2,0)).real();
1292 Cquqd1_1131i_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(2,0)).imag();
1293 Cquqd1_1133r_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(0,0)).real();
1294 Cquqd1_1133i_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(0,0)).imag();
1295 Cquqd1_1211r_LNP = (2*Cquqd1_00_LNP*YdL(0)*YuL(0,1)).real();
1296 Cquqd1_1211i_LNP = (2*Cquqd1_00_LNP*YdL(0)*YuL(0,1)).imag();
1297 Cquqd1_1221r_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(1,1)).real();
1298 Cquqd1_1221i_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(1,1)).imag();
1299 Cquqd1_1222r_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(0,1)).real();
1300 Cquqd1_1222i_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(0,1)).imag();
1301 Cquqd1_1231r_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(2,1)).real();
1302 Cquqd1_1231i_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(2,1)).imag();
1303 Cquqd1_1233r_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(0,1)).real();
1304 Cquqd1_1233i_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(0,1)).imag();
1305 Cquqd1_1311r_LNP = (2*Cquqd1_00_LNP*YdL(0)*YuL(0,2)).real();
1306 Cquqd1_1311i_LNP = (2*Cquqd1_00_LNP*YdL(0)*YuL(0,2)).imag();
1307 Cquqd1_1321r_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(1,2)).real();
1308 Cquqd1_1321i_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(1,2)).imag();
1309 Cquqd1_1322r_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(0,2)).real();
1310 Cquqd1_1322i_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(0,2)).imag();
1311 Cquqd1_1331r_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(2,2)).real();
1312 Cquqd1_1331i_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(2,2)).imag();
1313 Cquqd1_1333r_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(0,2)).real();
1314 Cquqd1_1333i_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(0,2)).imag();
1315 Cquqd1_2111r_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(1,0)).real();
1316 Cquqd1_2111i_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(1,0)).imag();
1317 Cquqd1_2112r_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(0,0)).real();
1318 Cquqd1_2112i_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(0,0)).imag();
1319 Cquqd1_2122r_LNP = (2*Cquqd1_00_LNP*YdL(1)*YuL(1,0)).real();
1320 Cquqd1_2122i_LNP = (2*Cquqd1_00_LNP*YdL(1)*YuL(1,0)).imag();
1321 Cquqd1_2132r_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(2,0)).real();
1322 Cquqd1_2132i_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(2,0)).imag();
1323 Cquqd1_2133r_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(1,0)).real();
1324 Cquqd1_2133i_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(1,0)).imag();
1325 Cquqd1_2211r_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(1,1)).real();
1326 Cquqd1_2211i_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(1,1)).imag();
1327 Cquqd1_2212r_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(0,1)).real();
1328 Cquqd1_2212i_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(0,1)).imag();
1329 Cquqd1_2222r_LNP = (2*Cquqd1_00_LNP*YdL(1)*YuL(1,1)).real();
1330 Cquqd1_2222i_LNP = (2*Cquqd1_00_LNP*YdL(1)*YuL(1,1)).imag();
1331 Cquqd1_2232r_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(2,1)).real();
1332 Cquqd1_2232i_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(2,1)).imag();
1333 Cquqd1_2233r_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(1,1)).real();
1334 Cquqd1_2233i_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(1,1)).imag();
1335 Cquqd1_2311r_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(1,2)).real();
1336 Cquqd1_2311i_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(1,2)).imag();
1337 Cquqd1_2312r_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(0,2)).real();
1338 Cquqd1_2312i_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(0,2)).imag();
1339 Cquqd1_2322r_LNP = (2*Cquqd1_00_LNP*YdL(1)*YuL(1,2)).real();
1340 Cquqd1_2322i_LNP = (2*Cquqd1_00_LNP*YdL(1)*YuL(1,2)).imag();
1341 Cquqd1_2332r_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(2,2)).real();
1342 Cquqd1_2332i_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(2,2)).imag();
1343 Cquqd1_2333r_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(1,2)).real();
1344 Cquqd1_2333i_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(1,2)).imag();
1345 Cquqd1_3111r_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(2,0)).real();
1346 Cquqd1_3111i_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(2,0)).imag();
1347 Cquqd1_3113r_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(0,0)).real();
1348 Cquqd1_3113i_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(0,0)).imag();
1349 Cquqd1_3122r_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(2,0)).real();
1350 Cquqd1_3122i_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(2,0)).imag();
1351 Cquqd1_3123r_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(1,0)).real();
1352 Cquqd1_3123i_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(1,0)).imag();
1353 Cquqd1_3133r_LNP = (2*Cquqd1_00_LNP*YdL(2)*YuL(2,0)).real();
1354 Cquqd1_3133i_LNP = (2*Cquqd1_00_LNP*YdL(2)*YuL(2,0)).imag();
1355 Cquqd1_3211r_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(2,1)).real();
1356 Cquqd1_3211i_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(2,1)).imag();
1357 Cquqd1_3213r_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(0,1)).real();
1358 Cquqd1_3213i_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(0,1)).imag();
1359 Cquqd1_3222r_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(2,1)).real();
1360 Cquqd1_3222i_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(2,1)).imag();
1361 Cquqd1_3223r_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(1,1)).real();
1362 Cquqd1_3223i_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(1,1)).imag();
1363 Cquqd1_3233r_LNP = (2*Cquqd1_00_LNP*YdL(2)*YuL(2,1)).real();
1364 Cquqd1_3233i_LNP = (2*Cquqd1_00_LNP*YdL(2)*YuL(2,1)).imag();
1365 Cquqd1_3311r_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(2,2)).real();
1366 Cquqd1_3311i_LNP = (Cquqd1_00_LNP*YdL(0)*YuL(2,2)).imag();
1367 Cquqd1_3313r_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(0,2)).real();
1368 Cquqd1_3313i_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(0,2)).imag();
1369 Cquqd1_3322r_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(2,2)).real();
1370 Cquqd1_3322i_LNP = (Cquqd1_00_LNP*YdL(1)*YuL(2,2)).imag();
1371 Cquqd1_3323r_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(1,2)).real();
1372 Cquqd1_3323i_LNP = (Cquqd1_00_LNP*YdL(2)*YuL(1,2)).imag();
1373 Cquqd1_3333r_LNP = (2*Cquqd1_00_LNP*YdL(2)*YuL(2,2)).real();
1374 Cquqd1_3333i_LNP = (2*Cquqd1_00_LNP*YdL(2)*YuL(2,2)).imag();
1375
1376 Cquqd8_1111r_LNP = (2*Cquqd8_00_LNP*YdL(0)*YuL(0,0)).real();
1377 Cquqd8_1111i_LNP = (2*Cquqd8_00_LNP*YdL(0)*YuL(0,0)).imag();
1378 Cquqd8_1121r_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(1,0)).real();
1379 Cquqd8_1121i_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(1,0)).imag();
1380 Cquqd8_1122r_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(0,0)).real();
1381 Cquqd8_1122i_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(0,0)).imag();
1382 Cquqd8_1131r_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(2,0)).real();
1383 Cquqd8_1131i_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(2,0)).imag();
1384 Cquqd8_1133r_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(0,0)).real();
1385 Cquqd8_1133i_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(0,0)).imag();
1386 Cquqd8_1211r_LNP = (2*Cquqd8_00_LNP*YdL(0)*YuL(0,1)).real();
1387 Cquqd8_1211i_LNP = (2*Cquqd8_00_LNP*YdL(0)*YuL(0,1)).imag();
1388 Cquqd8_1221r_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(1,1)).real();
1389 Cquqd8_1221i_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(1,1)).imag();
1390 Cquqd8_1222r_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(0,1)).real();
1391 Cquqd8_1222i_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(0,1)).imag();
1392 Cquqd8_1231r_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(2,1)).real();
1393 Cquqd8_1231i_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(2,1)).imag();
1394 Cquqd8_1233r_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(0,1)).real();
1395 Cquqd8_1233i_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(0,1)).imag();
1396 Cquqd8_1311r_LNP = (2*Cquqd8_00_LNP*YdL(0)*YuL(0,2)).real();
1397 Cquqd8_1311i_LNP = (2*Cquqd8_00_LNP*YdL(0)*YuL(0,2)).imag();
1398 Cquqd8_1321r_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(1,2)).real();
1399 Cquqd8_1321i_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(1,2)).imag();
1400 Cquqd8_1322r_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(0,2)).real();
1401 Cquqd8_1322i_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(0,2)).imag();
1402 Cquqd8_1331r_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(2,2)).real();
1403 Cquqd8_1331i_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(2,2)).imag();
1404 Cquqd8_1333r_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(0,2)).real();
1405 Cquqd8_1333i_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(0,2)).imag();
1406 Cquqd8_2111r_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(1,0)).real();
1407 Cquqd8_2111i_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(1,0)).imag();
1408 Cquqd8_2112r_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(0,0)).real();
1409 Cquqd8_2112i_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(0,0)).imag();
1410 Cquqd8_2122r_LNP = (2*Cquqd8_00_LNP*YdL(1)*YuL(1,0)).real();
1411 Cquqd8_2122i_LNP = (2*Cquqd8_00_LNP*YdL(1)*YuL(1,0)).imag();
1412 Cquqd8_2132r_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(2,0)).real();
1413 Cquqd8_2132i_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(2,0)).imag();
1414 Cquqd8_2133r_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(1,0)).real();
1415 Cquqd8_2133i_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(1,0)).imag();
1416 Cquqd8_2211r_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(1,1)).real();
1417 Cquqd8_2211i_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(1,1)).imag();
1418 Cquqd8_2212r_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(0,1)).real();
1419 Cquqd8_2212i_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(0,1)).imag();
1420 Cquqd8_2222r_LNP = (2*Cquqd8_00_LNP*YdL(1)*YuL(1,1)).real();
1421 Cquqd8_2222i_LNP = (2*Cquqd8_00_LNP*YdL(1)*YuL(1,1)).imag();
1422 Cquqd8_2232r_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(2,1)).real();
1423 Cquqd8_2232i_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(2,1)).imag();
1424 Cquqd8_2233r_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(1,1)).real();
1425 Cquqd8_2233i_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(1,1)).imag();
1426 Cquqd8_2311r_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(1,2)).real();
1427 Cquqd8_2311i_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(1,2)).imag();
1428 Cquqd8_2312r_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(0,2)).real();
1429 Cquqd8_2312i_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(0,2)).imag();
1430 Cquqd8_2322r_LNP = (2*Cquqd8_00_LNP*YdL(1)*YuL(1,2)).real();
1431 Cquqd8_2322i_LNP = (2*Cquqd8_00_LNP*YdL(1)*YuL(1,2)).imag();
1432 Cquqd8_2332r_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(2,2)).real();
1433 Cquqd8_2332i_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(2,2)).imag();
1434 Cquqd8_2333r_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(1,2)).real();
1435 Cquqd8_2333i_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(1,2)).imag();
1436 Cquqd8_3111r_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(2,0)).real();
1437 Cquqd8_3111i_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(2,0)).imag();
1438 Cquqd8_3113r_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(0,0)).real();
1439 Cquqd8_3113i_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(0,0)).imag();
1440 Cquqd8_3122r_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(2,0)).real();
1441 Cquqd8_3122i_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(2,0)).imag();
1442 Cquqd8_3123r_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(1,0)).real();
1443 Cquqd8_3123i_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(1,0)).imag();
1444 Cquqd8_3133r_LNP = (2*Cquqd8_00_LNP*YdL(2)*YuL(2,0)).real();
1445 Cquqd8_3133i_LNP = (2*Cquqd8_00_LNP*YdL(2)*YuL(2,0)).imag();
1446 Cquqd8_3211r_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(2,1)).real();
1447 Cquqd8_3211i_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(2,1)).imag();
1448 Cquqd8_3213r_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(0,1)).real();
1449 Cquqd8_3213i_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(0,1)).imag();
1450 Cquqd8_3222r_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(2,1)).real();
1451 Cquqd8_3222i_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(2,1)).imag();
1452 Cquqd8_3223r_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(1,1)).real();
1453 Cquqd8_3223i_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(1,1)).imag();
1454 Cquqd8_3233r_LNP = (2*Cquqd8_00_LNP*YdL(2)*YuL(2,1)).real();
1455 Cquqd8_3233i_LNP = (2*Cquqd8_00_LNP*YdL(2)*YuL(2,1)).imag();
1456 Cquqd8_3311r_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(2,2)).real();
1457 Cquqd8_3311i_LNP = (Cquqd8_00_LNP*YdL(0)*YuL(2,2)).imag();
1458 Cquqd8_3313r_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(0,2)).real();
1459 Cquqd8_3313i_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(0,2)).imag();
1460 Cquqd8_3322r_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(2,2)).real();
1461 Cquqd8_3322i_LNP = (Cquqd8_00_LNP*YdL(1)*YuL(2,2)).imag();
1462 Cquqd8_3323r_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(1,2)).real();
1463 Cquqd8_3323i_LNP = (Cquqd8_00_LNP*YdL(2)*YuL(1,2)).imag();
1464 Cquqd8_3333r_LNP = (2*Cquqd8_00_LNP*YdL(2)*YuL(2,2)).real();
1465 Cquqd8_3333i_LNP = (2*Cquqd8_00_LNP*YdL(2)*YuL(2,2)).imag();
1466
1467}
double CHud_33i_LNP
The dimension-6 operator coefficient (Imaginary part).
double CHq3_23i_LNP
The dimension-6 operator coefficient (Imaginary part).
double CHu_23i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Cqu8_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CHu_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Cqe_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CHud_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CdG_33i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Cqq1_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CdH_33i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Cqd8_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CHl1_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Cld_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Ced_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Ceu_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CuW_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Clq1_3323i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Clq3_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CdB_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Cqu1_3323i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Clq3_3323i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Cqd1_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CdH_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CHq1_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Cll_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Cuu_2333i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Cqu8_3323i_LNP
The dimension-6 operator coefficient (Imaginary part).
double CdW_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Cqu1_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CHd_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CdG_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Cqq1_2333i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Cquqd8_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Cqq3_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Cquqd8_3333i_LNP
The dimension-6 operator coefficient (Imaginary part).
double CHe_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Cqq3_2333i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Ceu_3323i_LNP
The dimension-6 operator coefficient (Imaginary part).
double CuG_33i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Clq1_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CdB_33i_LNP
The dimension-6 operator coefficient (Imaginary part).
double CHq3_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CuG_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CuH_33i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Cquqd1_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CuB_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Clu_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Cud1_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Cuu_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CuB_33i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Cquqd1_3333i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Cud8_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CdW_33i_LNP
The dimension-6 operator coefficient (Imaginary part).
double CuW_33i_LNP
The dimension-6 operator coefficient (Imaginary part).
double Clu_3323i_LNP
The dimension-6 operator coefficient (Imaginary part).
double getSMEFTCoeffEW(const std::string name) const
double CuH_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double CHq1_23i_LNP
The dimension-6 operator coefficient (Imaginary part).
double CHl3_33r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).
double Cdd_3333r_LNP
The dimension-6 operator coefficient (Real part and pure real operator).

◆ setParameter()

void NPSMEFTd6MFV::setParameter ( const std::string  name,
const double &  value 
)
protectedvirtual

Reimplemented from NPSMEFTd6General.

Definition at line 175 of file NPSMEFTd6MFV.cpp.

175 {
176 if (name.compare("CG_LNP") == 0) {
177 CG_LNP = value;
178 } else if (name.compare("CW_LNP") == 0) {
179 CW_LNP = value;
180 } else if (name.compare("CHG_LNP") == 0) {
181 CHG_LNP = value;
182 } else if (name.compare("CHW_LNP") == 0) {
183 CHW_LNP = value;
184 } else if (name.compare("CHB_LNP") == 0) {
185 CHB_LNP = value;
186 } else if (name.compare("CHWB_LNP") == 0) {
187 CHWB_LNP = value;
188 } else if (name.compare("CHD_LNP") == 0) {
189 CHD_LNP = value;
190 } else if (name.compare("CHbox_LNP") == 0) {
191 CHbox_LNP = value;
192 } else if (name.compare("CH_LNP") == 0) {
193 CH_LNP = value;
194 } else if (name.compare("CHl1_LNP") == 0) {
195 CHl1_LNP = value;
196 } else if (name.compare("CHl3_LNP") == 0) {
197 CHl3_LNP = value;
198 } else if (name.compare("CHe_LNP") == 0) {
199 CHe_LNP = value;
200 } else if (name.compare("Cll_aabb_LNP") == 0) {
201 Cll_aabb_LNP = value;
202 } else if (name.compare("Cll_abba_LNP") == 0) {
203 Cll_abba_LNP = value;
204 } else if (name.compare("Cee_LNP") == 0) {
205 Cee_LNP = value;
206 } else if (name.compare("Cle_LNP") == 0) {
207 Cle_LNP = value;
208 } else if (name.compare("CuH_0_LNP") == 0) {
209 CuH_0_LNP = value;
210 } else if (name.compare("CuH_u_LNP") == 0) {
211 CuH_u_LNP = value;
212 } else if (name.compare("CuH_d_LNP") == 0) {
213 CuH_d_LNP = value;
214 } else if (name.compare("CuG_0_LNP") == 0) {
215 CuG_0_LNP = value;
216 } else if (name.compare("CuG_u_LNP") == 0) {
217 CuG_u_LNP = value;
218 } else if (name.compare("CuG_d_LNP") == 0) {
219 CuG_d_LNP = value;
220 } else if (name.compare("CuW_0_LNP") == 0) {
221 CuW_0_LNP = value;
222 } else if (name.compare("CuW_u_LNP") == 0) {
223 CuW_u_LNP = value;
224 } else if (name.compare("CuW_d_LNP") == 0) {
225 CuW_d_LNP = value;
226 } else if (name.compare("CuB_0_LNP") == 0) {
227 CuB_0_LNP = value;
228 } else if (name.compare("CuB_u_LNP") == 0) {
229 CuB_u_LNP = value;
230 } else if (name.compare("CuB_d_LNP") == 0) {
231 CuB_d_LNP = value;
232 } else if (name.compare("CdH_0_LNP") == 0) {
233 CdH_0_LNP = value;
234 } else if (name.compare("CdH_u_LNP") == 0) {
235 CdH_u_LNP = value;
236 } else if (name.compare("CdH_d_LNP") == 0) {
237 CdH_d_LNP = value;
238 } else if (name.compare("CdG_0_LNP") == 0) {
239 CdG_0_LNP = value;
240 } else if (name.compare("CdG_u_LNP") == 0) {
241 CdG_u_LNP = value;
242 } else if (name.compare("CdG_d_LNP") == 0) {
243 CdG_d_LNP = value;
244 } else if (name.compare("CdW_0_LNP") == 0) {
245 CdW_0_LNP = value;
246 } else if (name.compare("CdW_u_LNP") == 0) {
247 CdW_u_LNP = value;
248 } else if (name.compare("CdW_d_LNP") == 0) {
249 CdW_d_LNP = value;
250 } else if (name.compare("CdB_0_LNP") == 0) {
251 CdB_0_LNP = value;
252 } else if (name.compare("CdB_u_LNP") == 0) {
253 CdB_u_LNP = value;
254 } else if (name.compare("CdB_d_LNP") == 0) {
255 CdB_d_LNP = value;
256 } else if (name.compare("CHq1_0_LNP") == 0) {
257 CHq1_0_LNP = value;
258 } else if (name.compare("CHq1_u_LNP") == 0) {
259 CHq1_u_LNP = value;
260 } else if (name.compare("CHq1_d_LNP") == 0) {
261 CHq1_d_LNP = value;
262 } else if (name.compare("CHq3_0_LNP") == 0) {
263 CHq3_0_LNP = value;
264 } else if (name.compare("CHq3_u_LNP") == 0) {
265 CHq3_u_LNP = value;
266 } else if (name.compare("CHq3_d_LNP") == 0) {
267 CHq3_d_LNP = value;
268 } else if (name.compare("CHu_0_LNP") == 0) {
269 CHu_0_LNP = value;
270 } else if (name.compare("CHu_u_LNP") == 0) {
271 CHu_u_LNP = value;
272 } else if (name.compare("CHd_0_LNP") == 0) {
273 CHd_0_LNP = value;
274 } else if (name.compare("CHd_d_LNP") == 0) {
275 CHd_d_LNP = value;
276 } else if (name.compare("CHud_ud_LNP") == 0) {
277 CHud_ud_LNP = value;
278 } else if (name.compare("Clq1_0_LNP") == 0) {
279 Clq1_0_LNP = value;
280 } else if (name.compare("Clq1_u_LNP") == 0) {
281 Clq1_u_LNP = value;
282 } else if (name.compare("Clq1_d_LNP") == 0) {
283 Clq1_d_LNP = value;
284 } else if (name.compare("Clq3_0_LNP") == 0) {
285 Clq3_0_LNP = value;
286 } else if (name.compare("Clq3_u_LNP") == 0) {
287 Clq3_u_LNP = value;
288 } else if (name.compare("Clq3_d_LNP") == 0) {
289 Clq3_d_LNP = value;
290 } else if (name.compare("Cqe_0_LNP") == 0) {
291 Cqe_0_LNP = value;
292 } else if (name.compare("Cqe_u_LNP") == 0) {
293 Cqe_u_LNP = value;
294 } else if (name.compare("Cqe_d_LNP") == 0) {
295 Cqe_d_LNP = value;
296 } else if (name.compare("Clu_0_LNP") == 0) {
297 Clu_0_LNP = value;
298 } else if (name.compare("Clu_u_LNP") == 0) {
299 Clu_u_LNP = value;
300 } else if (name.compare("Ceu_0_LNP") == 0) {
301 Ceu_0_LNP = value;
302 } else if (name.compare("Ceu_u_LNP") == 0) {
303 Ceu_u_LNP = value;
304 } else if (name.compare("Cld_0_LNP") == 0) {
305 Cld_0_LNP = value;
306 } else if (name.compare("Cld_d_LNP") == 0) {
307 Cld_d_LNP = value;
308 } else if (name.compare("Ced_0_LNP") == 0) {
309 Ced_0_LNP = value;
310 } else if (name.compare("Ced_d_LNP") == 0) {
311 Ced_d_LNP = value;
312 } else if (name.compare("Cqq1_00_LNP") == 0) {
313 Cqq1_00_LNP = value;
314 } else if (name.compare("Cqq1_0u_LNP") == 0) {
315 Cqq1_0u_LNP = value;
316 } else if (name.compare("Cqq1_0d_LNP") == 0) {
317 Cqq1_0d_LNP = value;
318 } else if (name.compare("Cqq1_u0_LNP") == 0) {
319 Cqq1_u0_LNP = value;
320 } else if (name.compare("Cqq1_uu_LNP") == 0) {
321 Cqq1_uu_LNP = value;
322 } else if (name.compare("Cqq1_ud_LNP") == 0) {
323 Cqq1_ud_LNP = value;
324 } else if (name.compare("Cqq1_d0_LNP") == 0) {
325 Cqq1_d0_LNP = value;
326 } else if (name.compare("Cqq1_du_LNP") == 0) {
327 Cqq1_du_LNP = value;
328 } else if (name.compare("Cqq1_dd_LNP") == 0) {
329 Cqq1_dd_LNP = value;
330 } else if (name.compare("Cqq3_00_LNP") == 0) {
331 Cqq3_00_LNP = value;
332 } else if (name.compare("Cqq3_0u_LNP") == 0) {
333 Cqq3_0u_LNP = value;
334 } else if (name.compare("Cqq3_0d_LNP") == 0) {
335 Cqq3_0d_LNP = value;
336 } else if (name.compare("Cqq3_u0_LNP") == 0) {
337 Cqq3_u0_LNP = value;
338 } else if (name.compare("Cqq3_uu_LNP") == 0) {
339 Cqq3_uu_LNP = value;
340 } else if (name.compare("Cqq3_ud_LNP") == 0) {
341 Cqq3_ud_LNP = value;
342 } else if (name.compare("Cqq3_d0_LNP") == 0) {
343 Cqq3_d0_LNP = value;
344 } else if (name.compare("Cqq3_du_LNP") == 0) {
345 Cqq3_du_LNP = value;
346 } else if (name.compare("Cqq3_dd_LNP") == 0) {
347 Cqq3_dd_LNP = value;
348 } else if (name.compare("Cuu_00_LNP") == 0) {
349 Cuu_00_LNP = value;
350 } else if (name.compare("Cuu_0u_LNP") == 0) {
351 Cuu_0u_LNP = value;
352 } else if (name.compare("Cuu_u0_LNP") == 0) {
353 Cuu_u0_LNP = value;
354 } else if (name.compare("Cuu_uu_LNP") == 0) {
355 Cuu_uu_LNP = value;
356 } else if (name.compare("Cdd_00_LNP") == 0) {
357 Cdd_00_LNP = value;
358 } else if (name.compare("Cdd_0d_LNP") == 0) {
359 Cdd_0d_LNP = value;
360 } else if (name.compare("Cdd_d0_LNP") == 0) {
361 Cdd_d0_LNP = value;
362 } else if (name.compare("Cdd_dd_LNP") == 0) {
363 Cdd_dd_LNP = value;
364 } else if (name.compare("Cud1_00_LNP") == 0) {
365 Cud1_00_LNP = value;
366 } else if (name.compare("Cud1_u0_LNP") == 0) {
367 Cud1_u0_LNP = value;
368 } else if (name.compare("Cud1_0d_LNP") == 0) {
369 Cud1_0d_LNP = value;
370 } else if (name.compare("Cud1_ud_LNP") == 0) {
371 Cud1_ud_LNP = value;
372 } else if (name.compare("Cud8_00_LNP") == 0) {
373 Cud8_00_LNP = value;
374 } else if (name.compare("Cud8_u0_LNP") == 0) {
375 Cud8_u0_LNP = value;
376 } else if (name.compare("Cud8_0d_LNP") == 0) {
377 Cud8_0d_LNP = value;
378 } else if (name.compare("Cud8_ud_LNP") == 0) {
379 Cud8_ud_LNP = value;
380 } else if (name.compare("Cqu1_00_LNP") == 0) {
381 Cqu1_00_LNP = value;
382 } else if (name.compare("Cqu1_u0_LNP") == 0) {
383 Cqu1_u0_LNP = value;
384 } else if (name.compare("Cqu1_d0_LNP") == 0) {
385 Cqu1_d0_LNP = value;
386 } else if (name.compare("Cqu1_0u_LNP") == 0) {
387 Cqu1_0u_LNP = value;
388 } else if (name.compare("Cqu1_uu_LNP") == 0) {
389 Cqu1_uu_LNP = value;
390 } else if (name.compare("Cqu1_du_LNP") == 0) {
391 Cqu1_du_LNP = value;
392 } else if (name.compare("Cqu8_00_LNP") == 0) {
393 Cqu8_00_LNP = value;
394 } else if (name.compare("Cqu8_u0_LNP") == 0) {
395 Cqu8_u0_LNP = value;
396 } else if (name.compare("Cqu8_d0_LNP") == 0) {
397 Cqu8_d0_LNP = value;
398 } else if (name.compare("Cqu8_0u_LNP") == 0) {
399 Cqu8_0u_LNP = value;
400 } else if (name.compare("Cqu8_uu_LNP") == 0) {
401 Cqu8_uu_LNP = value;
402 } else if (name.compare("Cqu8_du_LNP") == 0) {
403 Cqu8_du_LNP = value;
404 } else if (name.compare("Cqd1_00_LNP") == 0) {
405 Cqd1_00_LNP = value;
406 } else if (name.compare("Cqd1_u0_LNP") == 0) {
407 Cqd1_u0_LNP = value;
408 } else if (name.compare("Cqd1_d0_LNP") == 0) {
409 Cqd1_d0_LNP = value;
410 } else if (name.compare("Cqd1_0d_LNP") == 0) {
411 Cqd1_0d_LNP = value;
412 } else if (name.compare("Cqd1_ud_LNP") == 0) {
413 Cqd1_ud_LNP = value;
414 } else if (name.compare("Cqd1_dd_LNP") == 0) {
415 Cqd1_dd_LNP = value;
416 } else if (name.compare("Cqd8_00_LNP") == 0) {
417 Cqd8_00_LNP = value;
418 } else if (name.compare("Cqd8_u0_LNP") == 0) {
419 Cqd8_u0_LNP = value;
420 } else if (name.compare("Cqd8_d0_LNP") == 0) {
421 Cqd8_d0_LNP = value;
422 } else if (name.compare("Cqd8_0d_LNP") == 0) {
423 Cqd8_0d_LNP = value;
424 } else if (name.compare("Cqd8_ud_LNP") == 0) {
425 Cqd8_ud_LNP = value;
426 } else if (name.compare("Cqd8_dd_LNP") == 0) {
427 Cqd8_dd_LNP = value;
428 } else if (name.compare("Cquqd1_00_LNP") == 0) {
429 Cquqd1_00_LNP = value;
430 } else if (name.compare("Cquqd8_00_LNP") == 0) {
431 Cquqd8_00_LNP = value;
432 } else if (name.compare("Lambda_NP") == 0) {
433 Lambda_NP = value;
434 } else {
436 }
437}
std::string name
The name of the model.
Definition: Model.h:285
virtual void setParameter(const std::string name, const double &value)
A method to set the value of a parameter of the model.
double Lambda_NP
The new physics scale [GeV].

Member Data Documentation

◆ CdB_0_LNP

double NPSMEFTd6MFV::CdB_0_LNP = 0.
protected

Definition at line 85 of file NPSMEFTd6MFV.h.

◆ CdB_d_LNP

double NPSMEFTd6MFV::CdB_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{Hq}^{(1)})_{ij}\).

Definition at line 85 of file NPSMEFTd6MFV.h.

◆ CdB_u_LNP

double NPSMEFTd6MFV::CdB_u_LNP = 0.
protected

Definition at line 85 of file NPSMEFTd6MFV.h.

◆ Cdd_00_LNP

double NPSMEFTd6MFV::Cdd_00_LNP = 0.
protected

Definition at line 133 of file NPSMEFTd6MFV.h.

◆ Cdd_0d_LNP

double NPSMEFTd6MFV::Cdd_0d_LNP = 0.
protected

Definition at line 133 of file NPSMEFTd6MFV.h.

◆ Cdd_d0_LNP

double NPSMEFTd6MFV::Cdd_d0_LNP = 0.
protected

Definition at line 133 of file NPSMEFTd6MFV.h.

◆ Cdd_dd_LNP

double NPSMEFTd6MFV::Cdd_dd_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ud}^{(1)})_{ijkm}\).

Definition at line 133 of file NPSMEFTd6MFV.h.

◆ CdG_0_LNP

double NPSMEFTd6MFV::CdG_0_LNP = 0.
protected

Definition at line 79 of file NPSMEFTd6MFV.h.

◆ CdG_d_LNP

double NPSMEFTd6MFV::CdG_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{dW})_{ij}\).

Definition at line 79 of file NPSMEFTd6MFV.h.

◆ CdG_u_LNP

double NPSMEFTd6MFV::CdG_u_LNP = 0.
protected

Definition at line 79 of file NPSMEFTd6MFV.h.

◆ CdH_0_LNP

double NPSMEFTd6MFV::CdH_0_LNP = 0.
protected

Definition at line 76 of file NPSMEFTd6MFV.h.

◆ CdH_d_LNP

double NPSMEFTd6MFV::CdH_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{dG})_{ij}\).

Definition at line 76 of file NPSMEFTd6MFV.h.

◆ CdH_u_LNP

double NPSMEFTd6MFV::CdH_u_LNP = 0.
protected

Definition at line 76 of file NPSMEFTd6MFV.h.

◆ CdW_0_LNP

double NPSMEFTd6MFV::CdW_0_LNP = 0.
protected

Definition at line 82 of file NPSMEFTd6MFV.h.

◆ CdW_d_LNP

double NPSMEFTd6MFV::CdW_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{dB})_{ij}\).

Definition at line 82 of file NPSMEFTd6MFV.h.

◆ CdW_u_LNP

double NPSMEFTd6MFV::CdW_u_LNP = 0.
protected

Definition at line 82 of file NPSMEFTd6MFV.h.

◆ Ced_0_LNP

double NPSMEFTd6MFV::Ced_0_LNP = 0.
protected

Definition at line 121 of file NPSMEFTd6MFV.h.

◆ Ced_d_LNP

double NPSMEFTd6MFV::Ced_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qq}^{(1)})_{ijkm}\).

Definition at line 121 of file NPSMEFTd6MFV.h.

◆ Cee_LNP

double NPSMEFTd6MFV::Cee_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{le})_{ijkm}\).

Definition at line 58 of file NPSMEFTd6MFV.h.

◆ Ceu_0_LNP

double NPSMEFTd6MFV::Ceu_0_LNP = 0.
protected

Definition at line 115 of file NPSMEFTd6MFV.h.

◆ Ceu_u_LNP

double NPSMEFTd6MFV::Ceu_u_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ld})_{ijkm}\).

Definition at line 115 of file NPSMEFTd6MFV.h.

◆ CHd_0_LNP

double NPSMEFTd6MFV::CHd_0_LNP = 0.
protected

Definition at line 97 of file NPSMEFTd6MFV.h.

◆ CHd_d_LNP

double NPSMEFTd6MFV::CHd_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{Hud})_{ij}\).

Definition at line 97 of file NPSMEFTd6MFV.h.

◆ CHe_LNP

double NPSMEFTd6MFV::CHe_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ll})_{ijkm}\).

Definition at line 49 of file NPSMEFTd6MFV.h.

◆ CHl1_LNP

double NPSMEFTd6MFV::CHl1_LNP = 0.
protected

< Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{Hl}^{(1)})_{ij}\).

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{Hl}^{(3)})_{ij}\).

Definition at line 43 of file NPSMEFTd6MFV.h.

◆ CHl3_LNP

double NPSMEFTd6MFV::CHl3_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{He})_{ij}\).

Definition at line 46 of file NPSMEFTd6MFV.h.

◆ CHq1_0_LNP

double NPSMEFTd6MFV::CHq1_0_LNP = 0.
protected

Definition at line 88 of file NPSMEFTd6MFV.h.

◆ CHq1_d_LNP

double NPSMEFTd6MFV::CHq1_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{Hq}^{(3)})_{ij}\).

Definition at line 88 of file NPSMEFTd6MFV.h.

◆ CHq1_u_LNP

double NPSMEFTd6MFV::CHq1_u_LNP = 0.
protected

Definition at line 88 of file NPSMEFTd6MFV.h.

◆ CHq3_0_LNP

double NPSMEFTd6MFV::CHq3_0_LNP = 0.
protected

Definition at line 91 of file NPSMEFTd6MFV.h.

◆ CHq3_d_LNP

double NPSMEFTd6MFV::CHq3_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{Hu})_{ij}\).

Definition at line 91 of file NPSMEFTd6MFV.h.

◆ CHq3_u_LNP

double NPSMEFTd6MFV::CHq3_u_LNP = 0.
protected

Definition at line 91 of file NPSMEFTd6MFV.h.

◆ CHu_0_LNP

double NPSMEFTd6MFV::CHu_0_LNP = 0.
protected

Definition at line 94 of file NPSMEFTd6MFV.h.

◆ CHu_u_LNP

double NPSMEFTd6MFV::CHu_u_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{Hd})_{ij}\).

Definition at line 94 of file NPSMEFTd6MFV.h.

◆ CHud_ud_LNP

double NPSMEFTd6MFV::CHud_ud_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{lq}^{(1)})_{ijkm}\).

Definition at line 100 of file NPSMEFTd6MFV.h.

◆ Cld_0_LNP

double NPSMEFTd6MFV::Cld_0_LNP = 0.
protected

Definition at line 118 of file NPSMEFTd6MFV.h.

◆ Cld_d_LNP

double NPSMEFTd6MFV::Cld_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ed})_{ijkm}\).

Definition at line 118 of file NPSMEFTd6MFV.h.

◆ Cle_LNP

double NPSMEFTd6MFV::Cle_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{uH})_{ij}\).

Definition at line 61 of file NPSMEFTd6MFV.h.

◆ Cll_aabb_LNP

double NPSMEFTd6MFV::Cll_aabb_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ll})_{ijkm}\).

Definition at line 52 of file NPSMEFTd6MFV.h.

◆ Cll_abba_LNP

double NPSMEFTd6MFV::Cll_abba_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ee})_{ijkm}\).

Definition at line 55 of file NPSMEFTd6MFV.h.

◆ Clq1_0_LNP

double NPSMEFTd6MFV::Clq1_0_LNP = 0.
protected

Definition at line 103 of file NPSMEFTd6MFV.h.

◆ Clq1_d_LNP

double NPSMEFTd6MFV::Clq1_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{lq}^{(3)})_{ijkm}\).

Definition at line 103 of file NPSMEFTd6MFV.h.

◆ Clq1_u_LNP

double NPSMEFTd6MFV::Clq1_u_LNP = 0.
protected

Definition at line 103 of file NPSMEFTd6MFV.h.

◆ Clq3_0_LNP

double NPSMEFTd6MFV::Clq3_0_LNP = 0.
protected

Definition at line 106 of file NPSMEFTd6MFV.h.

◆ Clq3_d_LNP

double NPSMEFTd6MFV::Clq3_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qe})_{ijkm}\).

Definition at line 106 of file NPSMEFTd6MFV.h.

◆ Clq3_u_LNP

double NPSMEFTd6MFV::Clq3_u_LNP = 0.
protected

Definition at line 106 of file NPSMEFTd6MFV.h.

◆ Clu_0_LNP

double NPSMEFTd6MFV::Clu_0_LNP = 0.
protected

Definition at line 112 of file NPSMEFTd6MFV.h.

◆ Clu_u_LNP

double NPSMEFTd6MFV::Clu_u_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{eu})_{ijkm}\).

Definition at line 112 of file NPSMEFTd6MFV.h.

◆ Cqd1_00_LNP

double NPSMEFTd6MFV::Cqd1_00_LNP = 0.
protected

Definition at line 148 of file NPSMEFTd6MFV.h.

◆ Cqd1_0d_LNP

double NPSMEFTd6MFV::Cqd1_0d_LNP = 0.
protected

Definition at line 148 of file NPSMEFTd6MFV.h.

◆ Cqd1_d0_LNP

double NPSMEFTd6MFV::Cqd1_d0_LNP = 0.
protected

Definition at line 148 of file NPSMEFTd6MFV.h.

◆ Cqd1_dd_LNP

double NPSMEFTd6MFV::Cqd1_dd_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qd}^{(8)})_{ijkm}\).

Definition at line 148 of file NPSMEFTd6MFV.h.

◆ Cqd1_u0_LNP

double NPSMEFTd6MFV::Cqd1_u0_LNP = 0.
protected

Definition at line 148 of file NPSMEFTd6MFV.h.

◆ Cqd1_ud_LNP

double NPSMEFTd6MFV::Cqd1_ud_LNP = 0.
protected

Definition at line 148 of file NPSMEFTd6MFV.h.

◆ Cqd8_00_LNP

double NPSMEFTd6MFV::Cqd8_00_LNP = 0.
protected

Definition at line 151 of file NPSMEFTd6MFV.h.

◆ Cqd8_0d_LNP

double NPSMEFTd6MFV::Cqd8_0d_LNP = 0.
protected

Definition at line 151 of file NPSMEFTd6MFV.h.

◆ Cqd8_d0_LNP

double NPSMEFTd6MFV::Cqd8_d0_LNP = 0.
protected

Definition at line 151 of file NPSMEFTd6MFV.h.

◆ Cqd8_dd_LNP

double NPSMEFTd6MFV::Cqd8_dd_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{quqd}^{(1)})_{ijkm}\).

Definition at line 151 of file NPSMEFTd6MFV.h.

◆ Cqd8_u0_LNP

double NPSMEFTd6MFV::Cqd8_u0_LNP = 0.
protected

Definition at line 151 of file NPSMEFTd6MFV.h.

◆ Cqd8_ud_LNP

double NPSMEFTd6MFV::Cqd8_ud_LNP = 0.
protected

Definition at line 151 of file NPSMEFTd6MFV.h.

◆ Cqe_0_LNP

double NPSMEFTd6MFV::Cqe_0_LNP = 0.
protected

Definition at line 109 of file NPSMEFTd6MFV.h.

◆ Cqe_d_LNP

double NPSMEFTd6MFV::Cqe_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{lu})_{ijkm}\).

Definition at line 109 of file NPSMEFTd6MFV.h.

◆ Cqe_u_LNP

double NPSMEFTd6MFV::Cqe_u_LNP = 0.
protected

Definition at line 109 of file NPSMEFTd6MFV.h.

◆ Cqq1_00_LNP

double NPSMEFTd6MFV::Cqq1_00_LNP = 0.
protected

Definition at line 124 of file NPSMEFTd6MFV.h.

◆ Cqq1_0d_LNP

double NPSMEFTd6MFV::Cqq1_0d_LNP = 0.
protected

Definition at line 124 of file NPSMEFTd6MFV.h.

◆ Cqq1_0u_LNP

double NPSMEFTd6MFV::Cqq1_0u_LNP = 0.
protected

Definition at line 124 of file NPSMEFTd6MFV.h.

◆ Cqq1_d0_LNP

double NPSMEFTd6MFV::Cqq1_d0_LNP = 0.
protected

Definition at line 124 of file NPSMEFTd6MFV.h.

◆ Cqq1_dd_LNP

double NPSMEFTd6MFV::Cqq1_dd_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qq}^{(3)})_{ijkm}\).

Definition at line 124 of file NPSMEFTd6MFV.h.

◆ Cqq1_du_LNP

double NPSMEFTd6MFV::Cqq1_du_LNP = 0.
protected

Definition at line 124 of file NPSMEFTd6MFV.h.

◆ Cqq1_u0_LNP

double NPSMEFTd6MFV::Cqq1_u0_LNP = 0.
protected

Definition at line 124 of file NPSMEFTd6MFV.h.

◆ Cqq1_ud_LNP

double NPSMEFTd6MFV::Cqq1_ud_LNP = 0.
protected

Definition at line 124 of file NPSMEFTd6MFV.h.

◆ Cqq1_uu_LNP

double NPSMEFTd6MFV::Cqq1_uu_LNP = 0.
protected

Definition at line 124 of file NPSMEFTd6MFV.h.

◆ Cqq3_00_LNP

double NPSMEFTd6MFV::Cqq3_00_LNP = 0.
protected

Definition at line 127 of file NPSMEFTd6MFV.h.

◆ Cqq3_0d_LNP

double NPSMEFTd6MFV::Cqq3_0d_LNP = 0.
protected

Definition at line 127 of file NPSMEFTd6MFV.h.

◆ Cqq3_0u_LNP

double NPSMEFTd6MFV::Cqq3_0u_LNP = 0.
protected

Definition at line 127 of file NPSMEFTd6MFV.h.

◆ Cqq3_d0_LNP

double NPSMEFTd6MFV::Cqq3_d0_LNP = 0.
protected

Definition at line 127 of file NPSMEFTd6MFV.h.

◆ Cqq3_dd_LNP

double NPSMEFTd6MFV::Cqq3_dd_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{uu})_{ijkm}\).

Definition at line 127 of file NPSMEFTd6MFV.h.

◆ Cqq3_du_LNP

double NPSMEFTd6MFV::Cqq3_du_LNP = 0.
protected

Definition at line 127 of file NPSMEFTd6MFV.h.

◆ Cqq3_u0_LNP

double NPSMEFTd6MFV::Cqq3_u0_LNP = 0.
protected

Definition at line 127 of file NPSMEFTd6MFV.h.

◆ Cqq3_ud_LNP

double NPSMEFTd6MFV::Cqq3_ud_LNP = 0.
protected

Definition at line 127 of file NPSMEFTd6MFV.h.

◆ Cqq3_uu_LNP

double NPSMEFTd6MFV::Cqq3_uu_LNP = 0.
protected

Definition at line 127 of file NPSMEFTd6MFV.h.

◆ Cqu1_00_LNP

double NPSMEFTd6MFV::Cqu1_00_LNP = 0.
protected

Definition at line 142 of file NPSMEFTd6MFV.h.

◆ Cqu1_0u_LNP

double NPSMEFTd6MFV::Cqu1_0u_LNP = 0.
protected

Definition at line 142 of file NPSMEFTd6MFV.h.

◆ Cqu1_d0_LNP

double NPSMEFTd6MFV::Cqu1_d0_LNP = 0.
protected

Definition at line 142 of file NPSMEFTd6MFV.h.

◆ Cqu1_du_LNP

double NPSMEFTd6MFV::Cqu1_du_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qu}^{(8)})_{ijkm}\).

Definition at line 142 of file NPSMEFTd6MFV.h.

◆ Cqu1_u0_LNP

double NPSMEFTd6MFV::Cqu1_u0_LNP = 0.
protected

Definition at line 142 of file NPSMEFTd6MFV.h.

◆ Cqu1_uu_LNP

double NPSMEFTd6MFV::Cqu1_uu_LNP = 0.
protected

Definition at line 142 of file NPSMEFTd6MFV.h.

◆ Cqu8_00_LNP

double NPSMEFTd6MFV::Cqu8_00_LNP = 0.
protected

Definition at line 145 of file NPSMEFTd6MFV.h.

◆ Cqu8_0u_LNP

double NPSMEFTd6MFV::Cqu8_0u_LNP = 0.
protected

Definition at line 145 of file NPSMEFTd6MFV.h.

◆ Cqu8_d0_LNP

double NPSMEFTd6MFV::Cqu8_d0_LNP = 0.
protected

Definition at line 145 of file NPSMEFTd6MFV.h.

◆ Cqu8_du_LNP

double NPSMEFTd6MFV::Cqu8_du_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qd}^{(1)})_{ijkm}\).

Definition at line 145 of file NPSMEFTd6MFV.h.

◆ Cqu8_u0_LNP

double NPSMEFTd6MFV::Cqu8_u0_LNP = 0.
protected

Definition at line 145 of file NPSMEFTd6MFV.h.

◆ Cqu8_uu_LNP

double NPSMEFTd6MFV::Cqu8_uu_LNP = 0.
protected

Definition at line 145 of file NPSMEFTd6MFV.h.

◆ Cquqd1_00_LNP

double NPSMEFTd6MFV::Cquqd1_00_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{quqd}^{(8)})_{ijkm}\).

Definition at line 154 of file NPSMEFTd6MFV.h.

◆ Cquqd8_00_LNP

double NPSMEFTd6MFV::Cquqd8_00_LNP = 0.
protected

Definition at line 157 of file NPSMEFTd6MFV.h.

◆ CuB_0_LNP

double NPSMEFTd6MFV::CuB_0_LNP = 0.
protected

Definition at line 73 of file NPSMEFTd6MFV.h.

◆ CuB_d_LNP

double NPSMEFTd6MFV::CuB_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{dH})_{ij}\).

Definition at line 73 of file NPSMEFTd6MFV.h.

◆ CuB_u_LNP

double NPSMEFTd6MFV::CuB_u_LNP = 0.
protected

Definition at line 73 of file NPSMEFTd6MFV.h.

◆ Cud1_00_LNP

double NPSMEFTd6MFV::Cud1_00_LNP = 0.
protected

Definition at line 136 of file NPSMEFTd6MFV.h.

◆ Cud1_0d_LNP

double NPSMEFTd6MFV::Cud1_0d_LNP = 0.
protected

Definition at line 136 of file NPSMEFTd6MFV.h.

◆ Cud1_u0_LNP

double NPSMEFTd6MFV::Cud1_u0_LNP = 0.
protected

Definition at line 136 of file NPSMEFTd6MFV.h.

◆ Cud1_ud_LNP

double NPSMEFTd6MFV::Cud1_ud_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{ud}^{(8)})_{ijkm}\).

Definition at line 136 of file NPSMEFTd6MFV.h.

◆ Cud8_00_LNP

double NPSMEFTd6MFV::Cud8_00_LNP = 0.
protected

Definition at line 139 of file NPSMEFTd6MFV.h.

◆ Cud8_0d_LNP

double NPSMEFTd6MFV::Cud8_0d_LNP = 0.
protected

Definition at line 139 of file NPSMEFTd6MFV.h.

◆ Cud8_u0_LNP

double NPSMEFTd6MFV::Cud8_u0_LNP = 0.
protected

Definition at line 139 of file NPSMEFTd6MFV.h.

◆ Cud8_ud_LNP

double NPSMEFTd6MFV::Cud8_ud_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{qu}^{(1)})_{ijkm}\).

Definition at line 139 of file NPSMEFTd6MFV.h.

◆ CuG_0_LNP

double NPSMEFTd6MFV::CuG_0_LNP = 0.
protected

Definition at line 67 of file NPSMEFTd6MFV.h.

◆ CuG_d_LNP

double NPSMEFTd6MFV::CuG_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{uW})_{ij}\).

Definition at line 67 of file NPSMEFTd6MFV.h.

◆ CuG_u_LNP

double NPSMEFTd6MFV::CuG_u_LNP = 0.
protected

Definition at line 67 of file NPSMEFTd6MFV.h.

◆ CuH_0_LNP

double NPSMEFTd6MFV::CuH_0_LNP = 0.
protected

Definition at line 64 of file NPSMEFTd6MFV.h.

◆ CuH_d_LNP

double NPSMEFTd6MFV::CuH_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{uG})_{ij}\).

Definition at line 64 of file NPSMEFTd6MFV.h.

◆ CuH_u_LNP

double NPSMEFTd6MFV::CuH_u_LNP = 0.
protected

Definition at line 64 of file NPSMEFTd6MFV.h.

◆ Cuu_00_LNP

double NPSMEFTd6MFV::Cuu_00_LNP = 0.
protected

Definition at line 130 of file NPSMEFTd6MFV.h.

◆ Cuu_0u_LNP

double NPSMEFTd6MFV::Cuu_0u_LNP = 0.
protected

Definition at line 130 of file NPSMEFTd6MFV.h.

◆ Cuu_u0_LNP

double NPSMEFTd6MFV::Cuu_u0_LNP = 0.
protected

Definition at line 130 of file NPSMEFTd6MFV.h.

◆ Cuu_uu_LNP

double NPSMEFTd6MFV::Cuu_uu_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{dd})_{ijkm}\).

Definition at line 130 of file NPSMEFTd6MFV.h.

◆ CuW_0_LNP

double NPSMEFTd6MFV::CuW_0_LNP = 0.
protected

Definition at line 70 of file NPSMEFTd6MFV.h.

◆ CuW_d_LNP

double NPSMEFTd6MFV::CuW_d_LNP = 0.
protected

Coefficients of the MFV expansion of the dimension-6 operator coefficient \((C_{uB})_{ij}\).

Definition at line 70 of file NPSMEFTd6MFV.h.

◆ CuW_u_LNP

double NPSMEFTd6MFV::CuW_u_LNP = 0.
protected

Definition at line 70 of file NPSMEFTd6MFV.h.

◆ NNPSMEFTd6MFVVars

const int NPSMEFTd6MFV::NNPSMEFTd6MFVVars = 128+1
static

Definition at line 17 of file NPSMEFTd6MFV.h.

◆ NPSMEFTd6MFVVars

std::string NPSMEFTd6MFV::NPSMEFTd6MFVVars
static
Initial value:
= {
"CG_LNP","CW_LNP","CHG_LNP","CHW_LNP","CHB_LNP","CHWB_LNP","CHD_LNP","CHbox_LNP",
"CH_LNP","CHl1_LNP","CHl3_LNP","CHe_LNP","Cll_aabb_LNP","Cll_abba_LNP","Cee_LNP","Cle_LNP",
"CuH_0_LNP","CuH_u_LNP","CuH_d_LNP","CuG_0_LNP","CuG_u_LNP","CuG_d_LNP","CuW_0_LNP","CuW_u_LNP",
"CuW_d_LNP","CuB_0_LNP","CuB_u_LNP","CuB_d_LNP","CdH_0_LNP","CdH_u_LNP","CdH_d_LNP","CdG_0_LNP",
"CdG_u_LNP","CdG_d_LNP","CdW_0_LNP","CdW_u_LNP","CdW_d_LNP","CdB_0_LNP","CdB_u_LNP","CdB_d_LNP",
"CHq1_0_LNP","CHq1_u_LNP","CHq1_d_LNP","CHq3_0_LNP","CHq3_u_LNP","CHq3_d_LNP","CHu_0_LNP","CHu_u_LNP",
"CHd_0_LNP","CHd_d_LNP","CHud_ud_LNP","Clq1_0_LNP","Clq1_u_LNP","Clq1_d_LNP","Clq3_0_LNP","Clq3_u_LNP",
"Clq3_d_LNP","Cqe_0_LNP","Cqe_u_LNP","Cqe_d_LNP","Clu_0_LNP","Clu_u_LNP","Ceu_0_LNP","Ceu_u_LNP",
"Cld_0_LNP","Cld_d_LNP","Ced_0_LNP","Ced_d_LNP","Cqq1_00_LNP","Cqq1_0u_LNP","Cqq1_0d_LNP","Cqq1_u0_LNP",
"Cqq1_uu_LNP","Cqq1_ud_LNP","Cqq1_d0_LNP","Cqq1_du_LNP","Cqq1_dd_LNP","Cqq3_00_LNP","Cqq3_0u_LNP","Cqq3_0d_LNP",
"Cqq3_u0_LNP","Cqq3_uu_LNP","Cqq3_ud_LNP","Cqq3_d0_LNP","Cqq3_du_LNP","Cqq3_dd_LNP","Cuu_00_LNP","Cuu_0u_LNP",
"Cuu_u0_LNP","Cuu_uu_LNP","Cdd_00_LNP","Cdd_0d_LNP","Cdd_d0_LNP","Cdd_dd_LNP","Cud1_00_LNP","Cud1_u0_LNP",
"Cud1_0d_LNP","Cud1_ud_LNP","Cud8_00_LNP","Cud8_u0_LNP","Cud8_0d_LNP","Cud8_ud_LNP","Cqu1_00_LNP","Cqu1_u0_LNP",
"Cqu1_d0_LNP","Cqu1_0u_LNP","Cqu1_uu_LNP","Cqu1_du_LNP","Cqu8_00_LNP","Cqu8_u0_LNP","Cqu8_d0_LNP","Cqu8_0u_LNP",
"Cqu8_uu_LNP","Cqu8_du_LNP","Cqd1_00_LNP","Cqd1_u0_LNP","Cqd1_d0_LNP","Cqd1_0d_LNP","Cqd1_ud_LNP","Cqd1_dd_LNP",
"Cqd8_00_LNP","Cqd8_u0_LNP","Cqd8_d0_LNP","Cqd8_0d_LNP","Cqd8_ud_LNP","Cqd8_dd_LNP","Cquqd1_00_LNP","Cquqd8_00_LNP",
"Lambda_NP"
}

Definition at line 19 of file NPSMEFTd6MFV.h.


The documentation for this class was generated from the following files: